Optical image capturing system

ABSTRACT

A four-piece optical lens for capturing image and a four-piece optical module for capturing image are provided. In order from an object side to an image side, the optical lens along the optical axis includes a first lens with refractive power; a second lens with refractive power; a third lens with refractive power; and a fourth lens with positive refractive power; and at least one of the image-side surface and object-side surface of each of the four lens elements are aspheric. The optical lens can increase aperture value and improve the imagining quality for use in compact cameras.

CROSS-REFERENCE TO RELATED APPLICATION

This application claims the benefit of Taiwan Patent Application No. 104133275, filed on Oct. 8, 2015, in the Taiwan Intellectual Property Office, the disclosure of which is incorporated herein in its entirety by reference.

BACKGROUND OF THE INVENTION

1. Field of the Invention

The present disclosure relates to an optical image capturing system, and more particularly to a compact optical image capturing system which can be applied to electronic products.

2. Description of the Related Art

In recent years, with the rise of portable electronic devices having camera functionalities, the demand for an optical image capturing system is raised gradually. The image sensing device of ordinary photographing camera is commonly selected from charge coupled device (CCD) or complementary metal-oxide semiconductor sensor (CMOS Sensor). In addition, as advanced semiconductor manufacturing technology enables the minimization of pixel size of the image sensing device, the development of the optical image capturing system directs towards the field of high pixels. Therefore, the requirement for high imaging quality is rapidly raised.

The traditional optical image capturing system of a portable electronic device comes with different designs, and mainly includes a two-lens or a three-lens design. However, the requirement for the higher pixels and the requirement for a large aperture of an end user, like functionalities of micro filming and night view have been raised. The optical image capturing system in prior arts cannot meet the requirement of the higher order camera lens module.

Therefore, how to effectively increase quantity of incoming light of the optical lenses, and further improves imaging quality for the image formation, becomes a quite important issue.

SUMMARY OF THE INVENTION

The aspect of embodiment of the present disclosure directs to an optical image capturing system and an optical image capturing lens which use combination of refractive powers, convex and concave surfaces of four optical lenses (the convex or concave surface in the disclosure denotes the change of geometrical shape of an object-side surface or an image-side surface of each lens with different height from an optical axis) and by means of the mechanism element with a small wall thickness for positioning the lens elements, as well as the relative illumination to increase the quantity of incoming light of the optical image capturing system, and to improve imaging quality for image formation, on as to be applied to minimized electronic or narrow frame electronic products.

The term and its definition to the mechanism element parameter in the embodiment of the present invention are shown as below for further reference.

Please refer to FIG. 7. The optical image capturing system may include an image sensing module (not shown in figures including a substrate and a charge coupled device disposed on the substrate. The optical image capturing system may further include a first lens element positioning element 710 denoted by PE1 (Positioning Element 1). The first lens element positioning element 710 may include a basement 712 and a mirror base 714. The basement 712 has an opening accommodating space and is disposed on the substrate to facilitate the charge coupled device being positioned in the accommodating space. The mirror base 714 (may be integrated) is hollow and opaque, and has a cylinder 7141 and a basement 7142 which are connected with each other. The cylinder has a predetermined TPE1 (Thickness of Positioning Element 1), and a first through hole 7143 and a second through hole 7144 are respectively disposed at respective sides of the mirror base 714. The first through hole is connected to the cylinder and the second through hole is connected to the basement. A maximum value of the minimum side length of the basement vertical to the surface of the optical axis denoted by PhiD. The maximum hole diameter of the inner diameter of the second through hole is denoted by Phi2.

The optical image capturing system may further include a second lens element positioning element 720 denoted by PE2 (Positioning Element 2). The second lens element positioning element 720 may be accommodated in the mirror base of the first lens element positioning element and may include a positioning part 722 and a connecting part 724. The positioning part 722 is hollow and respectively disposed with a third through hole 7241 and a fourth through hole 7242 at two sides opposing to the direction of the optical axis. The third through hole 7241 is connected to the positioning part 722 and the fourth through hole 7242 is connected to the basement 7142. The positioning part 722 has a predetermined TPE2 (Thickness of Positioning Element 2) and directly contacts any of the lens elements of the present disclosure to position the accommodated lens elements and align the lens elements on the optical axis. The connecting part 724 is disposed outside the positioning part 722 and directly connected to the cylinder 7141, facilitating the second lens element 720 to be accommodated in the mirror base 714 of the first lens element positioning element and the optical image capturing system to correct the focal length and position the lens elements on the direction of the optical axis. The maximum outer diameter of the connecting part perpendicular to the surface of the optical axis is denoted by PhiC. The maximum hole diameter of the inner diameter of the fourth through hole 7242 is denoted by Phi4. The connecting part 724 may have screws, facilitating the second lens element positioning element 720 to be screwed to the mirror base 714 of the first lens element positioning element.

Any of the lens elements of the present disclosure may be directly disposed in the cylinder 7141 of the first lens element positioning element. Any of the chosen lens elements may be closer to the first through hole 7143 than the charge coupled device and face directly towards the charge coupled device. Alternatively, any of the chosen lens elements may be indirectly disposed in the first lens element positioning element 710 through the second lens element positioning element 720 and closer to the third through hole 7241 than the charge coupled device, and directly face towards the charge coupled device.

The term and its definition to the lens element parameter in the embodiment of the present invention are shown as below for further reference.

The lens element parameter related to a length or a height in the lens element

A height for image formation of the optical image capturing system is denoted by HOI. A height of the optical image capturing system is denoted by HOS. A distance from the object-side surface of the first lens element to the image-side surface of the second lens element is denoted by InTL. A distance from the image-side surface of the second lens element to an image plane is denoted by InB, and InTL+InB=HOS. A distance from an aperture stop (aperture) to an image plane is denoted by InS. A distance from the first lens element to the second lens element is denoted by IN12 (instance). A central thickness of the first lens element of the optical image capturing system on the optical axis is denoted by TP1 (instance).

The lens element parameter related to a material in the lens element

An Abbe number of the first lens element in the optical image capturing system is denoted by NA1 (instance). A refractive index of the first lens element is denoted by Nd1 (instance).

The lens element parameter related to a view angle in the lens element

A view angle is denoted by AF. Half of the view angle is denoted by HAF. A major light angle is denoted by MRA.

The lens element parameter related to exit/entrance pupil in the lens element.

An entrance pupil diameter of the optical image capturing system is denoted by HEP. The emergent pupil of the optical image capturing system means the image which passes though the aperture diaphragm and the lens element set behind the aperture diaphragm and then is formed in the image space. The emergent pupil is denoted by HXP. An entrance pupil diameter of the optical image capturing system is denoted by HEP. A maximum effective half diameter position of any surface of single lens element means the vertical height between the effective half diameter (EHD) and the optical axis where the incident light of the maximum view angle of the system passes through the farthest edge of the entrance pupil on the EHD of the surface of the lens element. For example, the maximum effective half diameter position of the object-side surface of the first lens element is denoted as EHD11. The maximum effective half diameter position of the image-side of the first lens element is denoted as EHD12. The maximum effective half diameter position of the object-side surface of the second lens element is denoted as EHD21. The maximum half effective half diameter position of the image-side surface of the second lens element is denoted as EHD22. The maximum effective half diameter position of any surfaces of the remaining lens elements of the optical image capturing system can be referred as mentioned above. The maximum effective diameter of the image-side surface which is nearest to the image plane of the optical image capturing system is denoted by PhiA, and the relationship is satisfied: PhiA=a double EHD. If the surface is aspheric, the cut-off point of the maximum effective diameter namely includes the cut-off point of the aspherical surface. An ineffective half diameter (IHD) position of any surface of single lens element means the surficial section of the cut-off point (if it is an aspheric surface, an point end of the aspherical coefficient is on the surface) of the maximum effective diameter extending from the same surface away from the optical axis. The maximum diameter of the image-side surface of the lens element which is nearest to the image plane of the optical image capturing system is denoted by PhiB, and the relationship is satisfied: PhiB a double (a maximum EHD+a maximum IHD)=PhiA+a double (a maximum IHD).

A maximum effective diameter of the image-side surface of the lens element which is nearest to the image plane (i.e. the image space) in the optical image capturing system is called the optical exit pupil and denoted by PhiA. If the optical exit pupil is on the image-side surface of the third lens element, it is denoted by PhiA3. If the optical exit pupil is on the image-side surface of the fourth lens element, it is denoted by PhiA4. If the optical exit pupil is on the image-side surface of the fifth lens element, it is denoted by PhiA5. If the optical exit pupil is on the image-side surface of the sixth lens element, it is denoted by PhiA6. If the optical image capturing system has lens elements with refractive power, the optical exit pupil is denoted based on the similar way as mentioned above. A pupil ratio of the optical image capturing system is denoted by PMR, and the relationship is satisfied: PMR=PhiA/HEP.

The lens element parameter related to an arc length of the element shape and an outline of surface

A length of outline curve of the maximum effective half diameter position of any surface of a single lens element refers to a length of outline curve from an axial point on the surface of the lens element to the maximum effective half diameter position of the surface along an outline of the surface of the lens element and is denoted as ARS. For example, the length of outline curve of the maximum effective half diameter position of the object-side surface of the first lens element is denoted as ARS11. The length of outline curve of the maximum effective half diameter position of the image-side surface of the first lens element is denoted as ARS12. The length of outline curve of the maximum effective half diameter position of the object-side surface of the second lens element is denoted as ARS21. The length of outline curve of the maximum effective half diameter position of the image-side surface of the second lens element is denoted as ARS22. The lengths of outline curve of the maximum effective half diameter position of any surface of the other lens elements in the optical image capturing system are denoted in the similar way.

A length of outline curve of a half of an pupil diameter (HEP) of any surface of a signal lens element refers to a length of outline curve of the half of the entrance pupil diameter (HEP) from an axial point on the surface of the lens element to a coordinate point of vertical height with a distance of the half of the entrance pupil diameter from the optical axis on the surface along the outline of the surface of the lens element and is denoted as ARE. For example, the length of the outline curve of the half of the entrance pupil diameter (HEP) of the object-side surface of the first lens element is denoted as ARE11. The length of the outline curve of the half of the entrance pupil diameter (HEP) of the image-side surface of the first lens element is denoted as ARE12. The length of the outline curve of the half of the entrance pupil diameter (HEP) of the object-side surface of the second lens element is denoted as ARE21. The length of the outline curve of the half of the entrance pupil diameter (HEP) of the image-side surface of the second lens element is denoted as ARE22. The lengths of outline curves of the half of the entrance pupil diameters (HEP) of any surface of the other lens elements in the optical image capturing system are denoted in the similar way.

The lens element parameter related to a depth of the lens element shape.

A horizontal distance in parallel with an optical axis from a maximum effective half diameter position to an axial point on the object-side surface of the fourth lens element is denoted by InRS41 (a depth of the maximum effective half diameter). A horizontal distance in parallel with an optical axis from a maximum effective half diameter position to an axial point on the image-side surface of the fourth lens element is denoted by InRS42 (the depth of the maximum effective half diameter).

The lens element parameter related to the lens element shape.

A critical point C is a tangent point on a surface of a specific lens element, and the tangent point is tangent to a plane perpendicular to the optical axis and the tangent point cannot be a crossover point on the optical axis. To follow the past, a distance perpendicular to the optical axis between a critical point C13 on the object-side surface of the third lens element and the optical axis is HVT31 (instance). A distance perpendicular to the optical axis between a critical point C32 on the image-side surface of the third lens element and the optical axis is HVT32 (instance). A distance perpendicular to the optical axis between a critical point C41 on the object-side surface of the fourth lens element and the optical axis is HVT41 (instance). A distance perpendicular to the optical axis between a critical point C42 on the image-side surface of the fourth lens element and the optical axis is HVT42 (instance). Distances perpendicular to the optical axis between critical points on the object-side surfaces or the image-side surfaces of other lens elements and the optical axis are denoted in the similar way described above.

The object-side surface of the fourth lens element has one inflection point IF411 which is nearest to the optical axis, and the sinkage value of the inflection point IF411 is denoted by SGI411. SGI411 is a horizontal shift distance in parallel with the optical axis from an axial point on the object-side surface of the fourth lens element to the inflection point which is nearest to the optical axis on the object-side surface of the fourth lens element. A distance perpendicular to the optical axis between the inflection point IF411 and the optical axis is HIF411 (instance). The image-side surface of the fourth lens element has one inflection point IF421 which is nearest to the optical axis and the sinkage value of the inflection point IF421 is denoted by SGI421 (instance). SGI421 is a horizontal shift distance in parallel with the optical axis from an axial point on the image-side surface of the fourth lens element to the inflection point which is nearest to the optical axis on the image-side surface of the fourth lens element. A distance perpendicular to the optical axis between the inflection point IF421 and the optical axis is HIF421 (instance).

The object-side surface of the fourth lens element has one inflection point IF412 which is the second nearest to the optical axis and the sinkage value of the inflection point IF412 is denoted by SGI412 (instance). SGI412 is a horizontal shift distance in parallel with the optical axis from an axial point on the object-side surface of the fourth lens element to the inflection point which is the second nearest to the optical axis on the object-side surface of the fourth lens element. A distance perpendicular to the optical axis between the inflection point IF412 and the optical axis is HIF412 (instance). The image-side surface of the fourth lens element has one inflection point IF422 which is the second nearest to the optical axis and the sinkage value of the inflection point IF422 is denoted by SGI422 (instance). SGI422 is a horizontal shift distance in parallel with the optical axis from an axial point on the image-side surface of the fourth lens element to the inflection point which is the fourth nearest to the optical axis on the image-side surface of the fourth lens element. A distance perpendicular to the optical axis between the inflection point IF4222 and the optical axis is HIF422 (instance).

The object-side surface of the fourth lens element has one inflection point IF413 which is the third nearest to the optical axis and the sinkage value of the inflection point IF413 is denoted by SGI413 (instance). SGI413 is a horizontal shift distance in parallel with the optical axis from an axial point on the object-side surface of the fourth lens element to the inflection point which is the third nearest to the optical axis on the object-side surface of the fourth d lens element. A distance perpendicular to the optical axis between the inflection point IF413 and the optical axis is HIF413 (instance). The image-side surface of the fourth lens element has one inflection point IF423 which is the third nearest to the optical axis and the sinkage value of the inflection point IF423 is denoted by SGI423 (instance). SGI423 is a horizontal shift distance in parallel with the optical axis from an axial point on the image-side surface of the fourth lens element to the inflection point which is the third nearest to the optical axis on the image-side surface of the fourth lens element. A distance perpendicular to the optical axis between the inflection point IF423 and the optical axis is HIF423 (instance).

The object-side surface of the fourth lens element has one inflection point IF414 which is the fourth nearest to the optical axis and the sinkage value of the inflection point IF414 is denoted by SGI414 (instance). SGI414 is a horizontal shift distance in parallel with the optical axis from an axial point on the object-side surface of the fourth lens element to the inflection point which is the fourth nearest to the optical axis on the object-side surface of the fourth lens element. A distance perpendicular to the optical axis between the inflection point IF414 and the optical axis is HIF414 (instance). The image-side surface of the fourth lens element has one inflection point IF424 which is the fourth nearest to the optical axis and the sinkage value of the inflection point IF424 is denoted by SGI424 (instance). SGI424 is a horizontal shift distance in parallel with the optical axis from an axial point on the image-side surface of the fourth lens element to the inflection point which is the fourth nearest to the optical axis on the image-side surface of the fourth lens element. A distance perpendicular to the optical axis between the inflection point IF424 and the optical axis is HIF424 (instance).

The inflection points on the object-side surfaces or the image-side surfaces of the other lens elements and the distances perpendicular to the optical axis thereof or the sinkage values thereof are denoted in the similar way described above.

The lens element parameter related to an aberration

Optical distortion for image formation in optical image capturing system is denoted by ODT. TV distortion for image formation in the optical image capturing system is denoted by TDT. Further, the range of the aberration offset for the view of image formation may be limited to 50%-100%. An offset of the spherical aberration is denoted by DFS. An offset of the coma aberration is denoted by DFC.

The lateral aberration of the stop is denoted as STA to assess the function of the specific optical image capturing system. The tangential fan or sagittal fan may be applied to calculate the STA of any view fields, and in particular, to calculate the STA of the max reference wavelength (e.g. 650 nm) and the minima reference wavelength (e.g. 470 nm) for serve as the standard of the optimal function. The aforementioned direction of the tangential fan can be further defined as the positive (overhead-light) and negative (lower-light) directions. The max operation wavelength, which passes through the STA, is defined as the image position of the specific view field, and the distance difference of two positions of image position of the view field between the max operation wavelength and the reference primary wavelength (e.g. wavelength of 555 nm), and the minimum operation wavelength, which passes through the STA, is defined as the image position of the specific view field, and STA of the max operation wavelength is defined as the distance between the image position of the specific view field of max operation wavelength and the image position of the specific view field of the reference primary wavelength (e.g. wavelength of 555 nm), and STA of the minimum operation wavelength is defined as the distance between the image position of the specific view field of the minimum operation wavelength and the image position of the specific view field of the reference primary wavelength (e.g. wavelength of 555 nm) are assessed the function of the specific optical image capturing system to be optimal. Both STA of the max operation wavelength and STA of the minimum operation wavelength on the image position of vertical height with a distance from the optical axis to 70% HOI (i.e. 0.7 HOI), which are smaller than 50 μm, are served as the sample. The numerical, which are smaller than 30 μm, are also served as the sample.

A maximum height for image formation on the image plane perpendicular to the optical axis in the optical image capturing system is denoted by HOI. A lateral aberration of the longest operation wavelength of a visible light of a positive direction tangential fan of the optical image capturing system passing through an edge of the entrance pupil and incident on the image plane by 0.7 HOI is denoted as PLTA. A lateral aberration of the shortest operation wavelength of a visible light of the positive direction tangential fan of the optical image capturing system passing through the edge of the entrance pupil and incident on the image plane by 0.7 HOI is denoted as PSTA. A lateral aberration of the longest operation wavelength of a visible light of a negative direction tangential fan of the optical image capturing system passing through the edge of the entrance pupil and incident on the image plane by 0.7 HOI is denoted as NLTA. A lateral aberration of the shortest operation wavelength of a visible light of a negative direction tangential fan of the optical image capturing system passing through the edge of the entrance pupil and incident on the image plane by 0.7 HOI is denoted as NSTA. A lateral aberration of the longest operation wavelength of a visible light of a sagittal fan of the optical image capturing system passing through the edge of the entrance pupil and incident on the image plane by 0.7 HOI is denoted as SLTA. A lateral aberration of the shortest operation wavelength of a visible light of the sagittal fan of the optical image capturing system passing through the edge of the entrance pupil and incident on the image plane by 0.7 HOI is denoted as SSTA.

The disclosure provides an optical image capturing system, an object-side surface or an image-side surface of the second lens element may have inflection points, such that the angle of incidence from each view field to the second lens element can be adjusted effectively and the optical distortion and the TV distortion can be corrected as well. Besides, the surfaces of the second lens element may have a better optical path adjusting ability to acquire better imaging quality.

The disclosure provides an optical image capturing system, in order from an object side to an image side including a first, second, third and fourth lens elements and an image plane. The first lens element has refractive power. An object-side surface and an object-side surface of the fourth lens element are both aspheric. Focal lengths of the first through fourth lens elements are f1, f2, f3 and f4 respectively. A focal length of the optical image capturing system is f. An entrance pupil diameter of the optical image capturing system is HEP. A distance on an optical axis from an object-side surface of the first lens element to the image plane is HOS. A distance on the optical axis from the object-side surface of the first lens element to the image-side surface of the fourth lens element is InTL. A maximum effective diameter of the image-side surface of the fourth lens element is PhiA4. A length of outline curve from an axial point on any surface of any one of the two lens elements to a coordinate point of vertical height with a distance of a half of the entrance pupil diameter from the optical axis on the surface along an outline of the surface is denoted as ARE. The following relations are satisfied: 1.2≦f/HEP≦10, 0/5≦HOS/f≦20, 0<PhiA4/InTL≦1.5 and 0.1≦2(ARE/HEP)≦2.0.

The disclosure provides another optical image capturing system, in order from an object side to an image side including a first lens element, a second lens element, a third lens element, a fourth lens element, an image plane, and a first lens element positioning element. The first lens element positioning element includes a mirror base which is hollow and opaque. The mirror base is connected to a cylinder and a basement. The cylinder is applied to accommodate the four lens elements and the basement is between the fourth lens element and the image plane. An outer periphery of the basement is greater than an outer periphery of the cylinder. A maximum value of the minimum side length of the basement perpendicular to the surface of the optical axis id denoted by PhiD. The first lens element has positive refractive power and may have a convex object-side surface near the optical axis. The second lens element has refractive power. The third lens element has refractive power. The fourth lens element has refractive power. Focal lengths of the four lens elements are f1, f2, f3 and f4 respectively. A focal length of the optical image capturing system is f. An entrance pupil diameter of the optical image capturing system is HEP. A distance on an optical axis from an object-side surface of the first lens element to the image plane is HOS. A distance on the optical axis from the object-side surface of the first lens element to the image-side surface of the second lens element is InTL. A length of outline curve from an axial point on any surface of any one of the four lens elements to a coordinate point of vertical height with a distance of a half of the entrance pupil diameter from the optical axis on the surface along an outline of the surface is denoted as ARE. The following relations are satisfied: 1.2≦f/HEP≦10, 0.5≦HOS/f≦20.0 mm<PhiD≦3.3 mm and 0.1≦2(ARE/HEP)≦2.0.

The disclosure provides another optical image capturing system, in order from an object side to an image side including a first lens element, a second lens element, a third lens element, a fourth lens element, an image plane, a first lens element positioning element and a second lens element positioning element. The first lens element positioning element includes a mirror base which is hollow and opaque. The mirror base is connected to a cylinder and a basement. The cylinder is applied to accommodate the four lens elements. The basement is between the fourth lens element and the image plane. An outer periphery of the basement is greater than an outer periphery of the cylinder. A maximum value of the minimum side length of the basement perpendicular to the surface of the optical axis is denoted by PhiD. The second lens element positioning element is accommodated in the mirror base and includes a positioning part and a connecting part. The positioning part is hollow and directly contacts and accommodates any of the four lens elements, facilitating the fourth lens elements to be aligned on the optical axis. The connecting part is disposed outside the positioning part and directly contacts an inner periphery of the cylinder. A maximum value of the connecting part perpendicular to the surface of the optical axis is denoted by PhiC. The first lens element has refractive power and has a convex surface near the optical axis. The second lens element has refractive power. The third lens element has refractive power. The fourth lens element has refractive power. At least one of the four lens elements has positive refractive power. Focal lengths of the four lens elements are f1, f2, f3, and f4, respectively. A focal length of the optical image capturing system is f. An entrance pupil diameter of the optical image capturing system is HEP. A distance on an optical axis from an object-side surface of the first lens element to the image plane is HOS. A distance on the optical axis from the object-side surface of the first lens element to the image-side surface of the fourth lens element is InTL. A maximum effective diameter of the image-side of the fourth lens element is denoted by PhiA4. A length of outline curve from an axial point on any surface of any one of the four lens elements to a coordinate point of vertical height with a distance of a half of the entrance pupil diameter from the optical axis on the surface along an outline of the surface is denoted as ARE. The following relations are satisfied: 1.2≦f/HEP≦0.5≦HOS/f≦20, PhiC<PhiD, 0 mm<PhiD≦3.3 mm and 0.1≦2(ARE/HEP)≦2.0.

The length of the outline curve of any surface of a signal lens element in the maximum effective half diameter position affects the functions of the surface aberration correction and the optical path difference in each view field. The longer outline curve may lead to a better function of aberration correction, but the difficulty of the production may become inevitable. Hence, the length of the outline curve of the maximum effective half diameter position of any surface of a signal lens element (ARS) has to be controlled, and especially, the ratio relations (ARS/TP) between the length of the outline curve of the maximum effective half diameter position of the surface (ARS) and the thickness of the lens element to which the surface belongs on the optical axis (TP) has to be controlled. For example, the length of the outline curve of the maximum effective half diameter position of the object-side surface of the first lens element is denoted as ARS11, and the thickness of the first lens element on the optical axis is TP1, and the ratio between both of them is ARS1/TP1. The length of the outline curve of the maximum effective half diameter position of the image-side surface of the first lens element is denoted as ARS12, and the ratio between ARS12 and TP1 is ARS12/TP1. The length of the outline curve of the maximum effective half diameter position of the object-side surface of the second lens element is denoted as ARS21, and the thickness of the second lens element on the optical axis is TP2, and the ratio between both of them is ARS21/TP2. The length of the outline curve of the maximum effective half diameter position of the image-side surface of the second lens element is denoted as ARS22, and the ratio between ARS22 and TP2 is ARS22/TP2. The ratio relations between the lengths of the outline curve of the maximum effective half diameter position of any surface of the other lens elements and the thicknesses of the lens elements to which the surfaces belong on the optical axis (TP) are denoted in the similar way.

The length of outline curve of half of an entrance pupil diameter of any surface of a single lens element especially affects the functions of the surface aberration correction and the optical path difference in each shared view field. The longer outline curve may lead to abetter function of aberration correction, but the difficulty of the production may become inevitable. Hence, the length of outline curve of half of an entrance pupil diameter of any surface of a single lens element has to be controlled, and especially, the ratio relationship between the length of outline curve of half of an entrance pupil diameter of any surface of a single lens element and the thickness on the optical axis has to he controlled. For example, the length of outline curve of the half of the entrance pupil diameter of the object-side surface of the first lens element is denoted as ARE11, and the thickness of the first lens element on the optical axis is TP1, and the ratio thereof is ARE11/TP1. The length of outline curve of the half of the entrance pupil diameter of the image-side surface of the first lens element is denoted as ARE12, and the thickness of the first lens element on the optical axis is TP1, and the ratio thereof is ARE12/TP1. The length of outline curve of the half of the entrance pupil diameter of the object-side surface of the first lens element is denoted as ARE21, and the thickness of the second lens element on the optical axis is TP2, and the ratio thereof is ARE21/TP2. The length of outline curve of the half of the entrance pupil diameter of the image-side surface of the second lens element is denoted as ARE22, and the thickness of the second lens element on the optical axis is TP2, and the ratio thereof is ARE22/TP2. The ratio relationship of the remaining lens elements of the optical image capturing system can be referred as mentioned above.

The optical image capturing system described above may be configured to form the image on the image sensing device which is shorter than 1/1.2 inch in diagonal length. The pixel size of the image sensing device is smaller than 1.4 micrometers (μm). Preferably the pixel size thereof is smaller than 1.12 micrometers (μm). The best pixel size thereof is smaller than 0.9 micrometers (μm). Furthermore, the optical image capturing system is applicable to the image sensing device with aspect ratio of 16:9.

The optical image capturing system described above is applicable to the demand of video recording with above millions or ten millions-pixels (e.g. 4K2K or the so-called UHD and QHD) and leads to a good imaging quality.

The height of optical system (HOS) may be reduced to achieve the minimization of the optical image capturing system when the absolute value of f1 is larger than f1(|f1|>f4).

When |f2|+|f3|>|f1|+|f4| are satisfied with above relations, at least one of the second through third lens elements may have weak positive refractive power or weak negative refractive power. The weak refractive power indicates that an absolute value of the focal length of a specific lens element is greater than 10. When at least one of the second through third lens elements has the weak positive refractive power, the positive refractive power of the first lens element can be shared, such that the unnecessary aberration will not appear too early. On the contrary, when at least one of the second and third lens elements has the weak negative refractive power, the aberration of the optical image capturing system can be corrected and fine tuned.

The fourth lens element may have positive refractive power. In addition, at least one of the object-side surface and the image-side surface of the fourth lens element may have at least one inflection point, such that the angle of incident with incoming light from an off-axis view field can be suppressed effectively and the aberration in the off-axis view field can be corrected further.

BRIEF DESCRIPTION OF IKE DRAWINGS

The detailed structure, operating principle and effects of the present disclosure will now be described in more details hereinafter with reference to the accompanying drawings that show various embodiments of the present disclosure as follows.

FIG. 1A is a schematic view of the optical image capturing system according to the first embodiment of the present application.

FIG. 1B is longitudinal spherical aberration curves, astigmatic field curves, and an optical distortion grid of the optical image capturing system in the order from left to right according to the first embodiment of the present application.

FIG. 1C is a lateral aberration diagram of tangential fan, sagittal fan, the longest operation wavelength and the shortest operation wavelength passing through an edge of the entrance pupil and incident on the image plane by 0.7 HOI according to the first embodiment of the present application.

FIG. 1D is a numerical figure of relative illumination of each view field on the image plane according to the first embodiment of the present application.

FIG. 2A is a schematic view of the optical image capturing system according to the second embodiment of the present application.

FIG. 2B is longitudinal spherical aberration curves, astigmatic field curves, and an optical distortion grid of the optical image capturing system in the order from left to right according to the second embodiment of the present application.

FIG. 2C is a lateral aberration diagram of tangential fan, sagittal fan, the longest operation wavelength and the shortest operation wavelength passing through an edge of the entrance pupil and incident on the image plane by 0.7 HOI according to the second embodiment of the present application.

FIG. 2D is a numerical figure of relative illumination of each view field on the image plane according to the second embodiment of the present application.

FIG. 3A is a schematic view of the optical image capturing system according to the third embodiment of the present application.

FIG. 3B is longitudinal spherical aberration curves, astigmatic field curves, and an optical distortion grid of the optical image capturing system in the order from left to right according to the third embodiment of the present application.

FIG. 3C is a lateral aberration diagram of tangential fan, sagittal fan, the longest operation wavelength and the shortest operation wavelength passing through an edge of the entrance pupil and incident on the image plane by 0.7 HOI according to the third embodiment of the present application.

FIG. 3D is a numerical figure of relative illumination of each view field on the image plane according to the third embodiment of the present application.

FIG. 4A is a schematic view of the optical image capturing system according to the fourth embodiment of the present application.

FIG. 4B is longitudinal spherical aberration curves, astigmatic field curves, and an optical distortion grid of the optical image capturing system in the order from left to right according to the fourth embodiment of the present application.

FIG. 4C is a lateral aberration diagram of tangential fan, sagittal fan, the longest operation wavelength and the shortest operation wavelength passing through an edge of the entrance pupil and incident on the image plane by 0.7 HOI according to the fourth embodiment of the present application.

FIG. 4D is a numerical figure of relative illumination of each view field on the image plane according to the fourth embodiment of the present application.

FIG. 5A is a schematic view of the optical image capturing system according to the fifth embodiment of the present application.

FIG. 5B is longitudinal spherical aberration curves, astigmatic field curves, and an optical distortion grid of the optical image capturing system in the order from left to right according to the fifth embodiment of the present application.

FIG. 5C is a lateral aberration diagram of tangential fan, sagittal fan, the longest operation wavelength and the shortest operation wavelength passing through an edge of the entrance pupil and incident on the image plane by 0.7 HOI according to the fifth embodiment of the present application.

FIG. 3D is a numerical figure of relative illumination of each view field on the image plane according to the fifth embodiment of the present application.

FIG. 6A is a schematic view of the optical image capturing system according to the sixth embodiment of the present application.

FIG. 6B is longitudinal spherical aberration curves, astigmatic field curves, and an optical distortion grid of the optical image capturing system in the order from left to right according to the sixth embodiment of the present application.

FIG. 6C is a lateral aberration diagram of tangential fan, sagittal fan, the longest operation wavelength and the shortest operation wavelength passing through an edge of the entrance pupil and incident on the image plane by 0.7 HOI according to the sixth embodiment of the present application.

FIG. 6D is a numerical figure of relative illumination of each view field on the image plane according to the sixth embodiment of the present application.

FIG. 7 is a schematic diagram illustrating the positions of a maximum effective diameter of the image-side surface of the fourth lens element PHiA4, a maximum diameter of the image-side surface of the fourth lens element PhiB, a maximum value of the minimum side length of the basement perpendicular to the surface of the optical axis denoted by PhiD, and a maximum outer diameter of the connection of the second lens element positioning element perpendicular to the surface of the optical axis of each embodiment of the present application.

DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS

Reference will now be made in detail to the exemplary embodiments of the present disclosure, examples of which are illustrated in the accompanying drawings. Therefore, it is to be understood that the foregoing is illustrative of exemplary embodiments and is not to be construed as limited to the specific embodiments disclosed, and that modifications to the disclosed exemplary embodiments, as well as other exemplary embodiments, are intended to be included within the scope of the appended claims. These embodiments are provided so that this disclosure will be thorough and complete, and will fully convey the inventive concept to those skilled in the art. The relative proportions and ratios of elements in the drawings may be exaggerated or diminished in size for the sake of clarity and convenience in the drawings, and such arbitrary proportions are only illustrative and not limiting in any way. The same reference numbers are used in the drawings and the description to refer to the same or like parts.

It will be understood that, although the terms ‘first’, ‘second’, ‘third’, etc., may be used herein to describe various elements, these elements should not be limited by these terms. The terms are used only for the purpose of distinguishing one component from another component. Thus, a first element discussed below could be termed a second element without departing from the teachings of embodiments. As used herein, the term “or” includes any and all combinations of one or more of the associated listed items.

An optical image capturing system, in order from an object side to an image side, includes a first, second, third and fourth lens elements with refractive power and an image plane. The optical image capturing system may further include an image sensing device which is disposed on an image plane.

The optical image capturing system may use three sets of wavelengths which are 486.1 nm, 587.5 nm and 656.2 nm, respectively, wherein 587.5 nm is served as the primary reference wavelength and a reference wavelength for retrieving technical features. The optical image capturing system may also use five sets of wavelengths which are 470 nm, 510 nm, 555 nm, 610 nm and 650 nm, respectively, wherein 555 nm is served as the primary reference wavelength and a reference wavelength for retrieving technical features.

A ratio of the focal length f of the optical image capturing system to a focal length fp of each of lens elements with positive refractive power is PPR. A ratio of the focal length f of the optical image capturing system to a focal length fn of each of lens elements with negative refractive power is NPR. A sum of the PPR of all lens elements with positive refractive power is ΣPPR. A sum of the NPR of all lens elements with negative refractive powers is ΣNPR. It is beneficial to control the total refractive power and the total length of the optical image capturing system when following conditions are satisfied: 0.5≦ΣPPR/|Σb NPR|≦4.5. Preferably, the following relation may be satisfied: 09.≦ΣPPR/|ΣNPR≦3.5.

The height of the optical image capturing system is HOS. It will facilitate the manufacturing of miniaturized optical image capturing system which may form images with ultra high pixels When the specific ratio value of HOS/f tends to 1.

A sum of a focal length fp of each lens element with positive refractive power is ΣPP. A sum of a focal length in of each lens element with negative refractive power is ΣNP. In one embodiment of the optical image capturing system of the present disclosure, the following relations are satisfied: 0<ΣPP≦200 and f4/ΣPP≦0.85. Preferably, the following relations may be satisfied: 0<ΣPP≦150 and 0.01≦f4/ΣPP≦0.7. Hereby, the miniaturization of the optical image capturing system can be maintained effectively, so as to be carried by lightweight portable electronic devices.

The optical image capturing system may further include an image sensing device which is disposed on an image plane. Half of a diagonal of an effective detection field of the image sensing device (imaging height or the maximum image height of the optical image capturing system) is HOI. A distance on an optical axis on the optical axis from the object-side surface of the first lens element to the image plane is HOS. The following relations are satisfied: HOS/HOI≦15 and 0.5≦HOS/f≦20.0. Preferably, the following relations may be satisfied: 1≦HOS/HOI≦10 and 1≦HOS/f≦15. Hereby, the miniaturization of the optical image capturing system can be maintained effectively, so as to be carried by lightweight portable electronic devices.

In addition, in the optical image capturing system of the disclosure, according to different requirements, at least one aperture stop may be arranged for reducing stray light and improving the imaging quality.

In the optical image capturing system of the disclosure, the aperture stop may be a front or middle aperture. The front aperture is the aperture stop between a photographed object and the first lens element. The middle aperture is the aperture stop between the first lens element and the image plane. If the aperture stop is the front aperture, a longer distance between the exit pupil and the image plane of the optical image capturing system can be formed, such that more optical elements can he disposed in the optical image capturing system and the efficiency of receiving images of the image sensing device can be raised. If the aperture stop is the middle aperture, the view angle of the optical image capturing system can be expended, such that the optical image capturing system has the same advantage that is owned by wide angle cameras. A distance from the aperture stop to the image plane is InS. The following relation is satisfied: 0.2≦InS/HOS≦1.1. Preferably, the following relation may be satisfied: 0.4≦InS/HOS≦1. Hereby, the miniaturization of the optical image capturing system can be maintained while the feature of the wild-angle lens element can be achieved.

In the optical image capturing system of the disclosure, a distance from the object-side surface of the first lens element to the image-side surface of the fourth lens element is InTL. A total central thickness of all lens elements with refractive power on the optical axis is ΣTP. The following relation is satisfied: 0.2≦ΣTP/InTL≦0.95. Preferably, the following relation may be satisfied: 0.2≦ΣTP/InTL≦0.9. Hereby, contrast ratio for the image formation in the optical image capturing system and defect-free rate for manufacturing the lens element can be given consideration simultaneously, and a proper back focal length is provided to dispose other optical components in the optical image capturing system.

A curvature radius of the object-side surface of the first lens element is R1. A curvature radius of the image-side surface of the first lens element is R2. The following relation is satisfied: 0.01≦|R1/R2|≦100. Preferably, the following relation may be satisfied: 0.01≦|R1/R2|≦60.

A curvature radius of the object-side surface of the fourth lens element is R1. A curvature radius of the image-side surface of the fourth lens element is R10. The following relation is satisfied: −200<(R7−R8)/(R7+R8)<30. Hereby, the astigmatism generated by the optical image capturing system can be corrected beneficially.

A distance between the first lens element and the second lens element on the optical axis is IN12. The following relation is satisfied: 0<IN12/f≦5.0. Preferably, the following relation may be satisfied: 0.01≦IN12/f≦4.0. Hereby, the chromatic aberration of the lens elements can be Improved, such that the performance can be increased.

A distance between the second lens element and the third lens element on the optical axis is IN23. The following relation is satisfied: 0<IN23/f≦5.0. Preferably, the following relation may be satisfied: 0.01≦IN23/f≦3.0. Hereby, the chromatic aberration of the lens elements can be improved, such that the performance can be increased.

A distance between the third lens element and the fourth lens element on the optical axis is IN34. The following relation is satisfied: 0<IN34/f≦5.0. Preferably, the following relation may be satisfied: 0.001≦IN34/f≦3.0. Hereby, the chromatic aberration of the lens elements can be improved, such that the performance can be increased.

Central thicknesses of the first lens element and the second lens element on the optical axis are TP1 and TP2, respectively. The following relation is satisfied: 1≦(TP1+IN12)//TP2≦20. Hereby, the sensitivity produced by the optical image capturing system can be controlled, and the performance can be increased.

Central thicknesses of the third lens element and the fourth lens element on the optical axis are TP3 and TP4, respectively. The following relation is satisfied: 0.2≦(TP4+IN34)/TP4≦20. Hereby, the sensitivity produced by the optical image capturing system can be controlled, and the performance can be increased.

A distance between the second lens element and the third lens element on the optical axis is IN23. A sum of the first through the fourth lens elements on the optical axis is ΣTP. The following, relation is satisfied: 0.01≦IN23/(TP2+IN23+TP3)≦0.9. Preferably, the following relation may be satisfied: 0.05≦IN23/(TP2+IN23+TP3)≦0.7. Hereby, the chromatic aberration of the lens elements can be improved, such that the performance can be increased.

In the optical image capturing system of the disclosure, a distance in parallel with an optical axis from a maximum effective diameter position to an axial point on the object-side surface of the fourth lens element is InRS41 (the InRS41 is positive if the horizontal displacement is toward the image-side surface, or the InRS41 is negative if the horizontal displacement is toward the object-side surface). A distance in parallel with an optical axis from a maximum effective diameter position to an axial point on the image-side surface of the fourth lens element is InRS42. A central thickness of the fourth lens element on the optical axis is TP4. The following relations are satisfied: −1 mm≦InRS41|1 mm, −1 mm≦INRS42≦1 mm, 1 mm≦|InRS41|+|InRS42|≦2 mm, 0.01≦|InRS41|/TP4≦10 and 0.01≦|InRS42|/TP4≦10. Hereby, the maximum effective half diameter of the image-side surface and the image-side surface of the fourth lens element can be controlled, and the chromatic aberration of the lens elements can be improved, such that the performance can be increased.

In the optical image capturing system of the disclosure, a distance in parallel with an optical axis from an inflection point on the object-side surface of the fourth lens element which is nearest to the optical axis to an axial point on the object-side surface of the fourth lens element is denoted by SGI411. A distance in parallel with an optical axis from an inflection point on the image-side surface of the fourth lens element which is nearest to the optical axis to an axial point on the image-side surface of the fourth lens element is denoted by SGI421. The following relations are satisfied: 0<SGI411/(SGI411+TP4)≦9, 0<SGI421/(SGI421+TP4)≦0.9. Preferably, the following relations may be satisfied: 0.01<SGI411/(SGI411+TP4)≦0.7, 0.01<SGI421/(SGI421+TP4)≦0.7.

A distance in parallel with the optical axis from the inflection point on the object-side surface of the fourth lens element Which is the second nearest to the optical axis to an axial point on the object-side surface of the fourth lens element is denoted by SGI412. A distance in parallel optical axis from an inflection point on the image-side surface of the fourth lens element which is the second nearest to the optical axis to an axial point on the image-side surface of the fourth lens element is denoted by SGI422. The following relations are satisfied: 0<SGI412/(SGI412+TP4)≦0.9, 0<SGI422 /(SGI422+TP4)≦0.9. Preferably, the following relations may be satisfied: 0.1≦SGI412 /(SGI412+TP4)≦0.8, 0.1≦SGI422/(SGI422+TP4)≦0.8.

A distance perpendicular to the optical axis between the inflection point on the object-side surface of the fourth h lens element which is the nearest to the optical axis and the optical axis is denoted by HIF411. A distance perpendicular to the optical axis between an axial point on the image-side surface of the fourth lens element and an inflection point on the image-side surface of the fourth lens element which is the nearest to the optical axis is denoted by HIF421. The following relations are satisfied: 0.01≦HIF411/HOI≦0.9, 0.01≦HIF421/HOI≦0.9. Preferably, the following relations may be satisfied: 0.09≦HIF411/HOI≦0.5, 0.09≦HIF421/HOI≦0.5.

A distance perpendicular to the optical axis between the inflection point on the object-side surface of the fourth lens element which is the second nearest to the optical axis and the optical axis is denoted by HIF412. A distance perpendicular to the optical axis between an axial point on the image-side surface of the fourth lens element and an inflection point on the image-side surface of the fourth lens element which is the second nearest to the optical axis is denoted by HIF422. The following relations are satisfied: 0.01≦HIF412/HOI≦0.9, 0.01≦HIF422/HOI≦0.9 m. Preferably, the following relations may be satisfied: 0.09≦HIF412/HOI≦0.8, 0.09≦HIF422/HOI≦0.8.

A distance perpendicular to the optical axis between the inflection point on the object-side surface of the fourth lens element which is the third nearest to the optical axis and the optical axis is denoted by HIF413. A distance perpendicular to the optical axis between an axial point on the image-side surface of the fourth lens element and an inflection point on the image-side surface of the fourth lens element which is the third nearest to the optical axis is denoted by HIF423. The following relations are satisfied: 0.001 mm≦|HIF413|≦5 mm, 0.001 mm≦|HIF423|≦5 mm. Preferably, the following relations may be satisfied: 0.1 mm≦|HIF423|≦3.5 mm, 0.1 mm≦|HIF413|≦3.5 mm.

A distance perpendicular to the optical axis between the inflection point on the object-side surface of the fourth lens element which is the fourth nearest to the optical axis and the optical axis is denoted by HIF414. A distance perpendicular to the optical axis between an axial point on the image-side surface of the fourth lens element and an inflection point on the image-side surface of the fourth lens element which is the fourth nearest to the optical axis is denoted by HIF424. The following relations are satisfied: 0.001 mm≦|HIF414|≦5 mm, 0.001 mm≦|HIF424|≦5. mm. Preferably, the following relations may be satisfied: 0.1 mm≦|HIF424|≦3.5 mm, 0.1 mm≦|HIF414≦3.5 mm.

In one embodiment of the optical image capturing system of the present disclosure, the chromatic aberration of the optical image capturing system can be corrected by alternatively arranging the lens elements with large Abbe number and small Abbe number.

The above Aspheric formula is:

z=ch2/[1+[1−(k+1)c2h2]0.5]+A4h4+A6h6+A8h8+A10h10+A12A12+A14h14+A16h16+A18h18+A20h20+ . . .   (1),

where z is a position value of the position along the optical axis and at the height h which reference to the surface apex; k is the conic coefficient, c is the reciprocal of curvature radius, and A4, A6, A8, A10, A12, A14, A16, A18, and A20 are high order aspheric coefficients.

The optical image capturing system provided by the disclosure, the lens elements may be made of glass or plastic material. If plastic material is adopted to produce the lens elements, the cost of manufacturing will be lowered effectively. If lens elements are made of glass, the heat effect can be controlled and the designed space arranged for the refractive power of the optical image capturing system can be increased. Besides, the object-side surface and the image-side surface of the first through fourth lens elements may be aspheric, so as to obtain more control variables. Comparing with the usage of traditional lens element made by glass, the number of lens elements used can be reduced and the aberration can be eliminated. Thus, the total height of the optical image capturing system can be reduced effectively.

In addition, in the optical image capturing system provided by the disclosure, if the lens element has a convex surface, the surface of the lens element adjacent to the optical axis is convex in principle. If the lens element has a concave surface, the surface of the lens element adjacent to the optical axis is concave in principle.

Besides, in the optical image capturing system of the disclosure, according to different requirements, at least one aperture may be arranged for reducing stray light and improving the imaging quality.

The optical image capturing system of the disclosure can be adapted to the optical image capturing system with automatic focus if required. With the features of a good aberration correction and a high quality of image formation, the optical image capturing system can be used in various application fields.

The optical image capturing system of the disclosure can include a driving module according to the actual requirements. The driving module may be coupled with the lens elements to enable the lens elements producing displacement. The driving module may be the voice coil motor (VCM) which is applied to move the lens to focus, or may be the optical image stabilization (OIS) which is applied to reduce the distortion frequency owing to the vibration of the lens while shooting.

At least one of the four lens elements of the optical image capturing system of the disclosure may further be designed as a light filtration element with a wavelength of less than 500 nm according to the actual requirement. The light filter element may be made by coating at least one surface of the specific lens element characterized of the filter function, and alternatively, may be made by the lens element per se made of the material which is capable of filtering short wavelength.

According to the above embodiments, the specific embodiments with figures are presented in detail as below.

The First Embodiment (Embodiment 1)

Please refer to FIG. 1A, FIG. 1B, FIG. 3 and FIG. 4. FIG. 1A is a schematic view of the optical image capturing system according to the first embodiment of the present application, FIG. 1B is longitudinal spherical aberration curves, astigmatic field curves, and an optical distortion curve of the optical image capturing system in the order from left to right according to the first embodiment of the present application, FIG. 1C is a lateral aberration diagram of tangential fan, sagittal fan, the longest operation wavelength and the shortest operation wavelength passing through an edge of the entrance pupil and incident on the image plane by 0.7 HOI according to the first embodiment of the present application, and FIG. 1D is a numerical figure of relative illumination of each view field on the image plane according to the first embodiment of the present application. As shown in FIG. 1A, in order from an object side to an image side, the optical image capturing system includes a first lens element 110, a second lens element 120, an aperture stop 100, a third lens element 130, a fourth lens element 140, an IR-bandstop filter 170, an image plane 180, and an image sensing device 190.

The first lens element 110 has negative refractive power and it is made of glass material. The first lens element 110 has a convex object-side surface 112 and a concave image-side surface 114, and both of the object-side surface 112 and the image-side surface 114 are aspheric. The length of outline curve of the maximum effective half diameter position of the object-side surface of the first lens element is denoted as ARS11. The length of outline curve of the maximum effective half diameter position of the image-side surface of the first lens element is denoted as ARS12. The length of outline curve of a half of an entrance pupil diameter (HEP) of the object-side surface of the first lens element is denoted as ARE11, and the length of outline curve of the half of the entrance pupil diameter (HEP) of the image-side surface of the first lens element is denoted as ARE12. The thickness of the first lens element on the optical axis is TP1.

A distance in parallel with an optical axis from an inflection point on the object-side surface of the first lens element which is nearest to the optical axis to an axial point on the object-side surface of the first lens element is denoted by SGI111. A distance in parallel with an optical axis from an inflection point on the image-side surface of the first lens element which is nearest to the optical axis to an axial point on the image-side surface of the first lens element is denoted by SGI121. The following relations are satisfied: SGI111=0 mm, SGI121=0 mm, |SGI111|/(⊕SGI111|+TP1)=0 and |SGI121|/(SGI121|+TP1)=0.

A distance perpendicular to the optical axis from the inflection point on the object-side surface of the first lens element which is nearest to the optical axis to an axial point on the object-side surface of the first lens element is denoted by HIF111. A distance perpendicular to the optical axis from the inflection point on the image-side surface of the first lens element which is nearest to the optical axis to an axial point on the image-side surface of the first lens element is denoted by HIF121. The following relations are satisfied: HIF111=0 mm, HIF121=0 mm, HIF111/HOI=0 and HIF121/HOI=0.

The second lens element 120 has positive refractive power and it is made of plastic material. The second lens element 120 has a concave object-side surface 122 and a convex image-side surface 124, and both of the object-side surface 122 and the image-side surface 124 are aspheric. The object-side surface 122 has an inflection point. The length of outline curve of the maximum effective half diameter position of the object-side surface of the second lens element is denoted as ARS21, and the length of outline curve of the maximum effective half diameter position of the image-side surface of the second lens element is denoted as ARS22. The length of outline curve of a half of an entrance pupil diameter (HEP) of the object-side surface of the second lens element is denoted as ARE21, and the length of outline curve of the half of the entrance pupil diameter (HEP) of the image-side surface of the second lens element is denoted as ARE22. The thickness of the second lens element on the optical axis is TP2.

A distance in parallel with an optical axis from an inflection point on the object-side surface of the second lens element which is nearest to the optical axis to an axial point on the object-side surface of the second lens element is denoted by SGI211. A distance in parallel with an optical axis from an inflection point on the image-side surface of the second lens element which is nearest to the optical axis to an axial point on the image-side surface of the second lens element is denoted by SGI221. The following relations are satisfied: SGI211=−0.13283 mm and |SGI211|/(SGI211|+TP2)=0.05045.

A distance perpendicular to the optical axis from the inflection point on the object-side surface of the second lens element which is nearest to the optical axis to an axial point on the object-side surface of the second lens element is denoted by HIF211. A distance perpendicular to the optical axis from the inflection point on the image-side surface of the second lens element which is nearest to the optical axis to an axial point on the image-side surface of the second lens element is denoted by HIF221. The following relations are satisfied: HIF211=2.10379 mm and HIF211/HOI=0.69478.

The third lens element 130 has negative refractive power and it is made of plastic material. The third lens element 130 has a concave object-side surface 132 and a concave image-side surface 134, and both of the object-side surface 132 and the image-side surface 134 are aspheric. The image-side surface 134 has an inflection point. The length of outline curve of the maximum effective half diameter position of the object-side surface of the third lens element is denoted as ARS31, and the length of outline curve of the maximum effective half diameter position of the image-side surface of the third lens element is denoted as ARS32. The length of outline curve of a half of an entrance pupil diameter (HEP) of the object-side surface of the third lens element is denoted as ARE31, and the length of outline curve of the half of the entrance pupil diameter (HEP) of the image-side surface of the third lens element is denoted as ARE32. The thickness of the third lens element on the optical axis is TP3.

A distance in parallel with an optical axis from an inflection point on the object-side surface of the third lens element which is nearest to the optical axis to an axial point on the object-side surface of the third lens element is denoted by SGI311. A distance in parallel with an optical axis from an inflection point on the image-side surface of the third lens element which is nearest to the optical axis to an axial point on the image-side surface of the third lens element is denoted by SGI321. The following relations are satisfied: SGI321=0.01218 mm:|SGI321|/(SGI321|+TP3)=0.03902.

A distance perpendicular to the optical axis between the inflection point on the object-side surface of the third lens element which is nearest to the optical axis and the optical axis is denoted by HIF311. A distance perpendicular to the optical axis from the inflection point on the image-side surface of the third lens element which is nearest to the optical axis to an axial point on the image-side surface of the third lens element is denoted by HIF321. The following relations are satisfied: HIF321=0.84373 mm and HIF321/HOI=0.27864.

The fourth lens element 140 has positive refractive power and it is made of plastic material. The fourth lens element 140 has a convex object-side surface 142 and a convex image-side surface 144, both of the object-side surface 142 and the image-side surface 144 are aspheric, and the image-side surface 144 has an inflection point. The length of outline curve of the maximum effective half diameter position of the object-side surface of the fourth lens element is denoted as ARS41, and the length of outline curve of the maximum effective half diameter position of the image-side surface of the fourth lens element is denoted as ARS42. The length of outline curve of a half of an entrance pupil diameter (HEP) of the object-side surface of the fourth lens element is denoted as ARE41, and the length of outline curve of the half of the entrance pupil diameter (HEP) of the image-side surface of the fourth lens element is denoted as ARE42. The thickness of the fourth lens element on the optical axis is TP4.

A distance in parallel with an optical axis from an inflection point on the object-side surface of the fourth lens element which is nearest to the optical axis to an axial point on the object-side surface of the fourth lens element is denoted by SGI411. A distance in parallel with an optical axis from an inflection point on the image-side surface of the fourth lens element which is nearest to the optical axis to an axial point on the image-side surface of the fourth lens element is denoted by SGI421. The following relations are satisfied: SGI411=0 mm, SGI421=−0.41627 mm, SGI411|/(SGI411|+TP4)=0 and |SGI421|/(|SGI421|+TP4)=0.25015.

A distance in parallel with an optical axis from an inflection point on the object-side surface of the fourth lens element which is the second nearest to the optical axis to an axial point on the object-side surface of the fourth lens element is denoted by SGI412. The following relations are satisfied: SGI412=0 mm and SGI412|/(SGI412+TP4)=0.

A distance perpendicular to the optical axis between the inflection point on the object-side surface of the fourth lens element Which is nearest to the optical axis and the optical axis is denoted by HIF411. The following relations are satisfied: HIF411=0 mm, HIF421=1.55079 mm, HIF411/HOI=0 and HIF421/HOI=0.51215.

A distance perpendicular to the optical axis between the inflection point on the image-side surface of the fourth lens element which is second nearest to the optical axis and the optical axis is denoted by HIF421. The following relations are satisfied: HIF412=0 mm and HIF412/HOI=0.

The IR-bandstop filter 170 is made of glass material without affecting the focal length of the optical image capturing system and it is disposed between the fourth lens element 140 and the image plane 180.

In the optical image capturing system of the first embodiment, a focal length of the optical image capturing system is f, an entrance pupil diameter of the optical image capturing system is HEP, and half of a maximal view angle of the optical image capturing system is HAF. The detailed parameters are shown as below: f=2.6841 mm, f/HEP=2.7959, HAF=70° and tan(HAF)=2.74759.

In the optical image capturing system of the first embodiment, a focal length of the first lens element 110 is f1 and a focal length of the fourth lens element 140 is f4. The following relations are satisfied: f1=−5.4534 mm,|f/f1|=0.4922, f4=2.7595 mm and |f1/f4|=1.9762.

In the optical image capturing system of the first embodiment, a focal length of the second lens element 120 is f2 and a focal length of the third lens element 130 is f3. The following relations are satisfied: |f2|f3|=13.2561 mm, |f1|+|f4|=8.2129 mm and |f2|+|f3|>|f1|+|f4

A ratio of the focal length f of the optical image capturing system to a focal length fp of each of lens elements with positive refractive power is PPR. A ratio of the focal length f of the optical image capturing, system to a focal length fn of each of lens elements with negative refractive power is NPR. In the optical image capturing system of the first embodiment, a sum of the PPR of all lens elements with positive refractive power is ΣPPR=|f/f2|+|f/f4|=1.25394. A sum of the NPR of all lens elements with negative refractive powers is ΣNPR=|f/f1|+|f/f2|=1.21490, ΣPPR/ΣNPR|=1.03213. The following relations are also satisfied: |f/f1|=0.49218, |f/f2|=0.2818, |f/f3|=0.72273 and |f/f4|=0.97267.

In the optical image capturing system of the first embodiment, a distance from the object-side surface 112 of the first lens element to the image-side surface 144 of the fourth lens element is InTL. A distance from the object-side surface 112 of the first lens element to the image plane 180 is HOS. A distance from an aperture 100 to an image plane 180 is InS. Half of a diagonal length of an effective detection field of the image sensing device 190 is HOI. A distance from the image-side surface 144 of the fourth lens element to an image plane 180 is InB. The following relations are satisfied: InTL+InB=HOS, HOS=18.74760 mm, HOI=3.088 mm, HOS/HOI=6.19141, HOS/f=6.9848; InTL/HOS=0.6605, InS=8.2310 mm and InS/HOS=0.4390.

In the optical image capturing system of the first embodiment, the sum of central thicknesses of all lens elements with refractive power on the optical axis is ΣTP. The following relations are satisfied: ΣTP=4.9656 mm and TP/InTL=0.4010. Hereby, contrast ratio for the image formation in the optical image capturing system and defect-free rate for manufacturing the lens element can be given consideration simultaneously, and a proper back focal length is provided to dispose other optical components in the optical image capturing system.

In the optical image capturing system of the first embodiment, a curvature radius of the object-side surface 112 of the first lens element is R1. A curvature radius of the image-side surface 114 of the first lens element is R2. The following relation is satisfied: |R1/R2=9.6100. Hereby, the first lens element may have proper strength of the positive refractive power, so as to avoid the longitudinal spherical aberration to increase too fast.

In the optical image capturing system of the first embodiment, a curvature radius of the object-side surface 142 of the fourth lens element is R7. A curvature radius of the image-side surface 144 of the fourth lens element is R8. The following relation is satisfied: (R7−R8)/(R7+R8)=−35.5932: Hereby, the astigmatism generated by the optical image capturing system can be corrected beneficially.

In the optical image capturing system of the first embodiment, a sum of focal lengths of all lens elements with positive refractive power is ΣPP. The following relations are satisfied: ΣPP=12.30183 mm and f4/ΣPP=0.22432. Hereby, it is favorable for allocating the positive refractive power of the fourth lens element 140 to other positive lens elements and the significant aberrations generated. In the process of moving the incident light can be suppressed.

In the optical image capturing system of the first embodiment, a sum of focal lengths of all lens elements with negative refractive power is ΣNP. The following relations are satisfied: ΣNP=−14.6405 mm and f1/ΣNP=0.59488. Hereby, it is favorable for allocating the negative refractive power of the fourth lens element 140 to other negative lens elements and the significant aberrations generated in the process of moving the incident light can be suppressed.

In the optical image capturing system of the first embodiment, a distance between the first lens element 110 and the second lens element 120 on the optical axis is IN12. The following relations are satisfied: IN12=4.5709 mm and IN12/f=1.70299. Hereby, the chromatic aberration of the lens elements can be improved, such that the performance can be increased.

In the optical image capturing system of the first embodiment, a distance between the second lens element 120 and the third lens element 130 on the optical axis is IN23. The following relations are satisfied: IN23=2.7524 mm and IN23/f=1.02548. Hereby, the chromatic aberration of the lens elements can be improved, such that the performance can be increased.

In the optical image capturing system of the first embodiment, a distance between the third lens element 130 and the fourth lens element 140 on the optical axis is IN32. The following relations are satisfied: IN34=0.0944 mm and IN34/f=0.03517. Hereby, the chromatic aberration of the lens elements can be improved, such that the performance can be increased.

In the optical image capturing system of the first embodiment, central thicknesses of the first lens element 110 and the second lens element 120 on the optical axis are TP1 and TP2, respectively. The following relations are satisfied: TP1=0.9179 mm. TP2=2.5000 mm, TP1/TP2=0.36715 and (TP1+IN12)/TP2=2.19552. Hereby, the sensitivity produced by the optical image capturing system can be controlled, and the performance can be increased.

In the optical image capturing system of the first embodiment, central thicknesses of the third lens element 130 and the fourth lens element 140 on the optical axis are TP3 and TP4, respectively. The following relations are satisfied: TP3=0.3 mm, TP4=1.2478 mm, TP3/TP4=0.24043 and (TP4+IN34)/TP3=4.47393. Hereby, the sensitivity produced by the optical image capturing system can be controlled, and the performance can be increased.

In the optical image capturing system of the e first embodiment, the following relations are satisfied: IN23/(TP2+IN23+TP3)=0.49572. Hereby, the aberration generated by the process of moving the incident light can be adjusted slightly layer upon layer, and the total height of the optical image capturing system can be reduced.

In the optical image capturing system of the first embodiment, a distance in parallel with an optical axis from a maximum effective diameter position to an axial point on the object-side surface 142 of the fourth lens element is InRS41. A distance in parallel with an optical axis from a maximum effective diameter position to an axial point on the image-side surface 144 of the fourth lens element is InRS42. A central thickness of the fourth lens element 140 is TP4. The following relations are satisfied: InRS41=0.2955 mm, InRS42=−0.4940 mm, |InRS41|+|InRS42|=0.7894 mm, |InRS41|/TP4=0.3679 and |InRS42|/TP4=0.39590. Hereby, it is favorable for manufacturing and forming the lens element and for maintaining the minimization for the optical image capturing system.

In the optical image capturing system of the first embodiment, a distance perpendicular to the optical axis between a critical point C41 on the object-side surface 142 of the fourth lens element and the optical axis is HVT41. A distance perpendicular to the optical axis between a critical point C42 on the image-side surface 144 of the fourth lens element and the optical axis is HVT42. The following relations are satisfied: HVT41=0 mm and HVT42=0 mm.

In the optical image capturing system of embodiment, the following relation is satisfied: HVT42/HOI=0.

In the optical image capturing system of the first embodiment, the following relation is satisfied: HVT42/HOI=0.

In the optical image capturing system of the first embodiment, an Abbe number of the first lens element is NA1. An Abbe number of the second lens element is NA2. An Abbe number of the third lens element is NA3. An Abbe number of the fourth lens element is NA4. The following relations are satisfied: |NA1-NA2=0.0351. Hereby, the chromatic aberration of the optical image capturing system can be corrected.

In the optical image capturing system of the first embodiment, TV distortion and optical distortion for image formation in the optical image capturing system are TDT and ODT, respectively. The following relations are satisfied: TDT=37.4846% and ODT=−55.3331%.

In the optical image capturing system of the first embodiment, a lateral aberration of the shortest operation wavelength of the positive direction tangential fan of the optical image capturing system passing through the edge of the aperture and incident on the image plane by 0.7 view field is denoted as PSTA, which is −0.018 mm. A lateral aberration of the longest operation wavelength of a positive direction tangential fan of the optical image capturing system passing through an edge of the aperture and incident on the image plane by 0.7 view field is denoted as PLTA, which is 0.010 mm. A lateral aberration of the shortest operation wavelength of a visible light of a negative direction tangential fan of the optical image capturing system passing through the edge of the aperture and incident on the image plane by 0.7 view field is denoted as NSTA, which is 0.003 mm. A lateral aberration of the longest operation wavelength of a negative direction tangential fan of the optical image capturing system passing through the edge of the aperture and incident on the image plane by 0.7 view field is denoted as NLTA, which is −0.003 mm. A lateral aberration of the shortest operation wavelength of the sagittal fan of the optical image capturing system passing through the edge of the aperture and incident on the image plane by 0.7 view field is denoted as SSTA, which is −0.010 mm. A lateral aberration of the longest operation wavelength of a sagittal fan of the optical image capturing system passing through the edge of the aperture and incident on the image plane by 0.7 view field is denoted as SLTA, which is 0.003 mm.

Please refer to FIG. 1D, which is a numerical figure of relative illumination of each view field on the image plane according to the first embodiment of the present application. The relative illuminations of the optical axis (0.0 view field), 0.1 view field, 0.2 view field, 0.3 view field, 0.4 view field, 0.5 view field, 0.6 view field, 0.7 view field, 0.8 view field, 0.9 view field and 1.0 view field are respectively denoted by R11, R12, R13, R14, R15, R16, R17, R18, R19, and R110. The relative illumination of the 0.9 view field is about 80%.

Please refer to FIG. 7. The optical image capturing system may include an image sensing module (not shown in figures) including a substrate and a charge coupled device disposed on the substrate. The optical image capturing system may further include a first lens element positioning element 710 denoted by PE1 (Positioning Element 1). The first lens element positioning element 710 may include a basement 712 and a mirror base 714. The basement 712 has an opening accommodating space and is disposed on the substrate to facilitate the charge coupled device being positioned in the accommodating space. The mirror base 714 (may be integrated) is hollow and opaque, and has a cylinder 7141 and a basement 7142 which are connected with each other. The cylinder has a predetermined TPE1 (Thickness of Positioning Element 1), and a first through hole 7143 and a second through hole 7144 are respectively disposed at respective sides of the mirror base 714. The first through hole is connected to the cylinder and the second through hole is connected to the basement. A maximum value of the minimum side length of the basement perpendicular to on the surface of the optical axis is denoted by PhiD, and PhiD=3.3 mm.

The optical image capturing system may further include a second lens element positioning element 720 denoted by PE2 (Positioning Element 2). The second lens element positioning element 720 may be accommodated in the mirror base of the first lens element positioning element and may include a positioning part 722 and a connecting part 724. The positioning part 722 is hollow and respectively disposed with a third through hole 7241 and a fourth through hole 7242 at two sides opposing to the direction of the optical axis. The third through hole 7241 is connected to the positioning part 722 and the fourth through hole 7242 is connected to the basement 7142. Any of the lens elements of the present disclosure may be directly disposed in the cylinder 7141 of the first lens element positioning element. Any of the chosen lens elements may he closer to the first through hole 7143 than the charge coupled device and face directly towards the charge coupled device. The maximum outer diameter of the connecting part perpendicular to the surface of the optical axis is denoted by PhiC, and PhiC=2.85. The maximum hole diameter of the inner diameter of the fourth through hole 7242 is denoted by Phi4. The connecting part 724 may have screws, facilitating the second lens element positioning element 720 to be screwed to the mirror base 714 of the first lens element positioning element.

Any of the chosen lens elements may be indirectly disposed in the first lens element positioning element 710 through the second lens element positioning element 720 and closer to the third through hole 7241 than the charge coupled device, and directly face towards the charge coupled device.

The fourth lens element 140 is the closest to the image plane of the present application, and the maximum diameter of the image-side surface of the fourth lens element is denoted by PhiA4, and the following relationship is satisfied: PhiA4=a double EHD42=1.767 mm. If the surface is aspheric, the cut-off point of the maximum effective diameter namely includes the cut-off point of the aspherical surface. An ineffective half diameter (IHD) position of the fourth lens element means the surficial section of the cut-off point of the maximum effective diameter extending from the same surface away from the optical axis. The fourth lens element 140 is the closest to the image plane of the present application, and the maximum diameter of the image-side surface of the fourth lens element is denoted by PhiB, and the following relationship is satisfied: PhiB=a double (a maximum EHD+a maximum IHD)=PhiA+a double (a maximum IHD).

A maximum effective diameter of the image-side surface of the lens element which is nearest to the image plane (i.e. the image space) in the optical image capturing system is called the optical exit pupil and denoted by PhiA. If the optical exit pupil is on the image-side surface of the fourth lens element, it is denoted by PhiA4. A pupil ratio of the optical image capturing system is denoted by PMR, and the relationship is satisfied: PMR=PhiA4/HEP=1.84337. A ratio to pupil and image is denoted by PMMR, and the relationship is satisfied: PMMR=Phi A4/ImgH=0.58355. A condensed ratio is denoted by PSMR, and relationship is satisfied: PSMR=PhiA4/InTL=0.14269.

Please refer to the following Table 1 and Table 2.

The detailed data of the optical image capturing system of the first embodiment is as shown in Table 1.

TABLE 1 Data of the optical image capturing system f = 2.6841 mm, f/HEP = 2.7959, HAF = 70 deg, tan(HAF) = 2.7475 Surface Focal # Curvature Radius Thickness Material Index Abbe # length 0 Object Plano At infinity 1 Lens 1 31.98102785 0.918 Glass 1.688 50.26 −5.453 2 3.327880578 4.571 3 Lens 2 −15.2556818 2.500 Plastic 1.647 22.46 9.542 4 −4.681543531 2.528 5 Ape. stop Plano 0.225 6 Lens 3 −2.453543123 0.300 Plastic 1.642 22.46 −3.714 7 127.8664454 0.094 8 Lens 4 2.697747363 1.248 Plastic 1.544 56.09 2.759 9 −2.853715061 0.725 10 IR-bandstop Plano 2.000 BK7_ 1.517 64.13 filter SCHOTT 11 Plano 3.640 12 Image plane Plano Reference wavelength (d-line) = 555 nm; shield position: The clear aperture of the third surface is 3.0 mm. As for the parameters of the aspheric surfaces of the first embodiment, reference is made to

Table 2

TABLE 2 Aspheric Coefficients Surface # 3 4 6 7 8 9 k = −2.918829E+01 −3.214789E+00 −1.504539E+01 −2.970417E+01 −1.613370E+01 −1.145951E+00 A4 = −9.004096E−04 −9.725260E−06   8.890018E−05   3.634454E−02   9.587367E−03 −4.742020E−03 A6 =   2.391364E−04 −8.096303E−05 −1.166688E−02 −3.060142E−02 −3.693991E−03   1.232422E−03 A8 = −2.421089E−05   7.787465E−07 −5.720942E−04   8.833265E−03   8.653836E−04   3.333400E−04 A10 =   1.716292E−06   3.517517E−07   8.305770E−04 −1.362695E−03 −7.093620E−05 −2.583094E−06 A12 =   0.000000E+00   0.000000E+00   0.000000E+00   0.000000E+00   0.000000E+00   0.000000E+00

The numerical related to the length of outline curve is shown according to table 1 and table 2.

First embodiment (Reference wavelength = 555 nm) ARE 2(ARE/HEP) ARE/TP ARE 1/2(HEP) value ARE-1/2(HEP) % TP (%) 11 0.480 0.480 0.000 100.00% 0.918 52.30% 12 0.480 0.482 0.002 100.35% 0.918 52.48% 21 0.480 0.480 0.000 100.02% 2.500 19.20% 22 0.480 0.481 0.001 100.17% 2.500 19.23% 31 0.480 0.482 0.002 100.49% 0.300 160.78% 32 0.480 0.480 0.000 100.00% 0.300 160.00% 41 0.480 0.482 0.002 100.42% 1.248 38.63% 42 0.480 0.482 0.002 100.47% 1.248 38.65% ARS (ARS/EHD) ARS/TP ARS EHD value ARS-EHD % TP (%) 11 5.943 5.978 0.035 100.58% 0.918 651.27% 12 3.236 4.439 1.204 137.20% 0.918 483.66% 21 3.000 3.007 0.007 100.24% 2.500 120.29% 22 2.855 2.983 0.128 104.49% 2.500 119.33% 31 1.061 1.079 0.017 101.61% 0.300 359.54% 32 1.293 1.292 −0.001 99.95% 0.300 430.77% 41 1.642 1.676 0.034 102.06% 1.248 134.30% 42 1.767 1.859 0.092 105.21% 1.248 148.98%

Table 1 is the detailed structure data to the first embodiment in FIG. 1A, wherein the unit of the curvature radius, the thickness, the distance, and the focal length is millimeters (mm). Surfaces 0-16 illustrate the surfaces from the object side to the image plane in the optical image capturing system. Table 2 is the aspheric coefficients of the first embodiment, wherein k is the conic coefficient in the aspheric surface formula, and A1-A20 are the first to the twentieth order aspheric surface coefficient. Besides, the tables in the following embodiments are referenced to the schematic view and the aberration graphs, respectively, and definitions of parameters in the tables are equal to those in the Table 1 and the Table 2, so the repetitious details will not be given here.

The Second Embodiment (Embodiment 2)

Please refer to FIG. 2A, FIG. 2B, FIG. 2C, and FIG. 2D. FIG. 2A is a schematic view of the optical image capturing system according to the second embodiment of the present application, FIG. 2B is longitudinal spherical aberration curves, astigmatic field curves, and an optical distortion curve of the optical image capturing system in the order from left to right according to the second embodiment of the present application, FIG. 2C is a lateral aberration diagram of tangential fan, sagittal fan, the longest operation wavelength and the shortest operation wavelength passing through an edge of the entrance pupil and incident on the image plane by 0.7 HOI according to the second embodiment of the present application, and FIG. 2D is a numerical figure of relative illumination of each view field on the image plane according to the second embodiment of the present application. As shown in FIG. 2A, in order from an object side to an image side, the optical image capturing system includes a first lens element 210, an aperture stop 200, a second lens element 220, a third lens element 230, a fourth lens element 240, an image plane 280, and an image sensing device 290.

The first lens element 210 has positive refractive power and it is made of plastic material. The first lens element 210 has a convex object-side surface 212 and a concave image-side surface 214, and both of the object-side surface 212 and the image-side surface 214 are aspheric and have an inflection point.

The second lens element 220 has positive refractive power and it is made of plastic material. The second lens element 220 has a convex object-side surface 222 and a convex image-side surface 224, and both of the object-side surface 222 and the image-side surface 224 are aspheric. The object-side surface 222 has an inflection point.

The third lens element 230 has negative refractive power and it is made of plastic material. The third lens element 230 has a concave object-side surface 232 and a convex image-side surface 234, and both of the object-side surface 232 and the image-side surface 234 are aspheric and have an inflection point.

The fourth lens element 240 has positive refractive power and it is made of plastic material. The fourth lens element 240 has a convex object-side surface 242 and a concave image-side surface 244, and both of the object-side surface 242 and the image-side surface 244 are aspheric and have an inflection point.

The IR-bandstop filter 270 is made of glass material without affecting the focal length of the optical image capturing system and it is disposed between the fourth lens element 240 and the image plane 280.

In the optical image capturing system of the second embodiment, the first, second and third lens elements are all positive lens elements and the focal lengths are respectively f1, f2, and f3. A sum of focal lengths of all lens elements with positive refractive power is ΣPP. The following relation is satisfied: ΣPP=f1+f2+f3 mm. Hereby, it is favorable for allocating the positive refractive power of a single lens element to other positive lens elements and the significant aberrations generated in the process of moving the incident light can be suppressed.

In the optical image capturing system of the second embodiment, a sum of focal lengths of all lens elements with negative refractive power is ΣNP. The following relation is satisfied: ΣNP=f4.

Please refer to the following Table 3 and Table 4.

The detailed data of the optical image capturing system of the second embodiment is as shown in Table 3.

TABLE 3 Data of the optical image capturing system f = 1.3219 mm; f/HEP = 2.05; HAF(tan) = 37.5115; tan(HAF) = 0.7676 Surface Abbe Focal # Curvature Radius Thickness Material Index # length 0 Object Plano 600 1 Lens 1 0.875196402 0.215 Plastic 1.642 22.46 11.076 2 0.90057215 0.064 3 Ape. stop Plano 0.030 4 Lens 2 0.814507073 0.296 Plastic 1.544 55.96 1.233 5 −3.394585334 0.159 6 Lens 3 −0.504765567 0.181 Plastic 1.642 22.46 −1.802 7 −1.015227124 0.056 8 Lens 4 0.374064886 0.214 Plastic 1.544 55.96 1.948 9 0.460507202 0.141 10 IR-bandstop Plano 0.145 BK7_ 1.517 64.13 filter SCHOTT 11 Plano 0.362 12 Image plane Plano Reference wavelength (d-line) = 555 nm; shield position: The clear aperture of the first surface is 0.375 mm. The clear aperture of the third surface is 0.295 mm. The clear aperture of the ninth surface is 0.778 mm. As for the parameters of the aspheric surfaces of the second embodiment, reference is made to Table 4.

TABLE 4 Aspheric Coefficients Surface # 1 2 4 5 k = 3.059860E+00 1.541511E+00 −1.419042E−01 9.323232E+00 A4 = −1.245184E+00 −1.533114E+00 −1.186679E+00 4.144582E−01 A6 = −3.844188E+00 −1.063483E+01 −4.401033E+00 −9.059084E+01 A8 = 8.142175E+01 4.156158E+01 3.051438E+01 2.151346E+03 A10 = −1.700955E+03 1.298229E+03 −7.993670E+02 −3.448173E+04 A12 = 1.354958E+04 −4.059303E+03 −6.590046E+03 3.292731E+05 A14 = −4.907557E+04 −2.423335E+05 1.619100E+05 −1.829152E+06 A16 = 4.929382E+04 −1.661634E+06 −7.106195E+05 5.658325E+06 A18 = 0.000000E+00 0.000000E+00 0.000000E+00 −7.758274E+06 A20 = 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 Surface # 6 7 8 9 k = −9.988011E+00 5.564944E−01 −4.471308E+00 −1.652829E+00 A4 = −7.447057E+00 −6.647712E+00 −3.112884E+00 −2.209832E+00 A6 = 1.004511E+02 6.560260E+01 1.646010E+01 −8.734263E+00 A8 = −2.394109E+03 −1.599136E+02 −1.666847E+02 1.238090E+02 A10 = 3.663820E+04 −4.959919E+03 1.122427E+03 −6.770854E+02 A12 = −3.193430E+05 7.289516E+04 −3.925278E+03 2.228931E+03 A14 = 1.737807E+06 −4.163032E+05 4 965550E+03 −4.682441E+03 A16 = −5.575953E+06 1.107395E+06 8.954645E+03 6.119357E+03 A18 = 7.896588E+06 −1.150017E+06 −3.510074E+04 −4.520455E+03 A20 = 0.000000E+00 0.000000E+00 3.084419E+04 1.433566E+03

In the second embodiment, the presentation of the aspheric surface formula is similar to that in the first embodiment. Besides, the definitions of parameters in following tables are equal to those in the first embodiment, so the repetitious details will not be given here.

The following contents may be deduced from Table 3 and Table 4.

Second embodiment (Primary reference wavelength = 555 nm) InRS41 InRS42 HVT41 HVT42 ODT % TDT % 0.03561 0.05562 0.40208 0.53316 2.99194 0.49744 | f/f1 | | f/f2 | | f/f3 | | f/f4 | | f1/f2 | | f2/f3 | 0.11509 1.03376 0.70759 0.65448 8.98232 0.68448 Σ PPR Σ NPR Σ PPR/| Σ NPR | Σ PP Σ NP f1/Σ PP 2.72200 0.70759 3.84686 14.25690  −1.80151  0.77689 f4/Σ NP IN12/f IN23/f IN34/f TP3/f TP4/f −1.08115  0.07337 0.12471 0.04397 0.14217 0.16756 InTL HOS HOS/HOI InS/HOS InTL/HOS Σ TP/InTL 1.21411 1.86200 1.81128 0.85043 0.65205 0.74587 (TP1 + IN12)/TP2 (TP4 + IN34)/TP3 TP1/TP2 TP3/TP4 IN23/(TP2 + IN23 + TP3) 1.04305 1.48778 0.72685 0.84851 0.24997 | InRS41 |/TP4 | InRS42 |/TP4 HVT42/HOI HVT42/HOS PhiA4/InTL PhiA4/HOI 0.1667  0.2604  0.5186  0.2863   1.355726  1.601167 PhiA4 PhiB PhiC PhiD RI9 PhiA4/HEP  1.646 mm  2.046 mm 2.746 mm 3.196 mm 40% 2.58251 PSTA PLTA NSTA NLTA SSTA SLTA −0.004 mm −0.001 mm 0.012 mm 0.002 mm −0.010 mm 0.003 mm

The following contents may be deduced from Table 3 and Table 4.

Second embodiment (Primary reference wavelength = 555 nm) HIF111 0.3436 HIF111/HOI 0.3342 SGI111 0.0597 | SGI111 |/(| SGI111 | + TP1) 0.2173 HIF121 0.2399 HIF121/HOI 0.2333 SGI121 0.0272 | SGI121 |/(| SGI121 | + TP1) 0.1125 HIF211 0.2311 HIF211/HOI 0.2248 SGI211 0.0292 | SGI211 |/(| SGI211 | + TP2) 0.0899 HIF311 0.2961 HIF311/HOI 0.2881 SGI311 −0.0916 | SGI311 |/(| SGI311 | + TP3) 0.3357 HIF321 0.3102 HIF321/HOI 0.3018 SGI321 −0.0736 | SGI321 |/(| SGI321 | + TP3) 0.2888 HIF411 0.1914 HIF411/HOI 0.1861 SGI411 0.0375 | SGI411 |/(| SGI411 | + TP4) 0.1494 HIF421 0.2488 HIF421/HOI 0.2420 SGI421 0.0551 | SGI421 |/(| SGI421 | + TP4) 0.2049

The numerical related to the length of outline curve is shown according to table 3 and table 4.

Second embodiment Reference wavelength = 555 nm ARE 2(ARE/HEP) ARE/TP ARE 1/2(HEP) value ARE-1/2(HEP) % TP (%) 11 0.320 0.324 0.00449 101.40% 0.215 150.93% 12 0.307 0.310 0.00248 100.81% 0.215 144.16% 21 0.315 0.319 0.00342 101.09% 0.296 107.78% 22 0.320 0.323 0.00323 101.01% 0.296 109.28% 31 0.320 0.341 0.02128 106.65% 0.181 188.29% 32 0.320 0.332 0.01221 103.82% 0.181 183.29% 41 0.320 0.328 0.00765 102.39% 0.214 153.39% 42 0.320 0.330 0.01030 103.22% 0.214 154.63% ARS (ARS/EHD) ARS/TP ARS EHD value ARS-EHD % TP (%) 11 0.375 0.382 0.00671 101.79% 0.215 177.56% 12 0.307 0.310 0.00248 100.81% 0.215 144.16% 21 0.315 0.319 0.00342 101.09% 0.296 107.78% 22 0.345 0.351 0.00563 101.63% 0.296 118.55% 31 0.368 0.395 0.02743 107.46% 0.181 218.05% 32 0.435 0.454 0.01873 104.30% 0.181 250.62% 41 0.603 0.625 0.02206 103.66% 0.214 292.66% 42 0.778 0.833 0.05462 107.02% 0.214 389.84%

The Third Embodiment (Embodiment 3)

Please refer to FIG. 3A, FIG. 3B, FIG. 3C, and 3D. FIG. 3A is a schematic view of the optical image capturing system according to the third embodiment of the present application, FIG. 3B is longitudinal spherical aberration curves, astigmatic field curves, and an optical distortion curve of the optical image capturing system in the order from left to right according to the third embodiment of the present application, FIG. 3C is a lateral aberration diagram of tangential fan, sagittal fan, the longest operation wavelength and the shortest operation wavelength passing through an edge of the entrance pupil and incident on the image plane by 0.7 HOI according to the third embodiment of the present application, and FIG. 3D is a numerical figure of relative illumination of each view field on the image plane according to the third embodiment of the present application. As shown in FIG. 3A, in order from an object side to an image side, the optical image capturing system includes a first lens element 310, an aperture stop 300, a second lens element 320, a third lens element 330, a fourth lens element 340, an IR-bandstop filter 370, an image plane 380, and an image sensing device 390.

The first lens element 310 has negative refractive power and it is made of plastic material. The first lens element 310 has a convex object-side surface 312 and a concave image-side surface 314, and both of the object-side surface 312 and the image-side surface 314 are aspheric and have an inflection point.

The second lens element 320 has positive refractive power and it is made of plastic material. The second lens element 320 has a convex object-side surface 322 and a convex image-side surface 324, and both of the object-side surface 322 and the image-side surface 324 are aspheric and have an inflection point.

The third lens element 330 has negative refractive power and it is made of plastic material. The third lens element 330 has a concave object-side surface 332 and a convex image-side surface 334, and both of the object-side surface 332 and the image-side surface 334 are aspheric and have an inflection point.

The fourth lens element 340 has positive refractive power and it is made of plastic material. The fourth lens element 340 has a convex object-side surface 342 and a concave image-side surface 344, and both of the object-side surface 342 and the image-side surface 344 are aspheric and have an inflection point.

The IR-bandstop filter 370 is made of glass material without affecting the focal length of the optical image capturing system and it is disposed between the fourth lens element 340 and the image plane 380.

In the optical image capturing system of the third embodiment, the second and the fourth lens elements are positive lens elements, and focal lengths are respectively f2 and f4. A sum of focal lengths of all lens elements with positive refractive power is ΣPP=f2+f4. Hereby, it is favorable for allocating the positive refractive power of a single lens element to other positive lens elements and the significant aberrations generated in the process of moving the incident light can be suppressed.

In the optical image capturing system of the third embodiment, focal lengths of the first and the third lens element are respectively f1 and f3. A sum of focal lengths of all lens elements with negative refractive power is ΣNP. The following relation is satisfied: ΣNP=f1+f3. Hereby, it is favorable for allocating the negative refractive power of a single lens element to other negative lens elements.

Please refer to the following Table 5 and Table 6.

The detailed data of the optical image capturing system of the third embodiment is as shown in Table 5.

TABLE 5 Data of the optical image capturing system f = 1.2859 mm; f/HEP = 2.0; HAF = 37.522 deg; tan(HAF) = 0.7679 Focal Surface# Curvature Radius Thickness Material Index Abbe # length 0 Object Plano At infinity 1 Lens 1 0.868009978 0.215 Plastic 1.642 22.46 −12.498 2 0.707624917 0.053 3 Ape. stop Plano 0.050 4 Lens 2 0.567584804 0.333 Plastic 1.544 55.96 0.959 5 −5.414461091 0.147 6 Lens 3 −0.48514482 0.181 Plastic 1.642 22.46 −1.482 7 −1.125341151 0.043 8 Lens 4 0.357017786 0.214 Plastic 1.544 55.96 1.944 9 0.424171789 0.112 10 IR-bandstop Plano 0.145 BK7_ 1.517 64.13 filter SCHOTT 11 Plano 0.370 12 Image plane Plano Reference wavelength (d-line) = 555 nm; shield position: The clear aperture of the first surface is 0.383 mm. The clear aperture of the fifth surface is 0.400 mm. The clear aperture of the ninth surface is 0.706 mm. As for the parameters of the aspheric surfaces of the third embodiment, reference is made to Table 6.

TABLE 6 Aspheric Coefficients Surface # 1 2 4 5 6 7 k = 3.011046E+00 8.496212E−01 −1.996345E−01 9.323232E+00 −1.427646E+01 −3.467853E−01 A4 = −1.584874E+00 −1.575769E+00 −2.453892E+00 1.750966E+00 −5.779057E+00 −8.789686E+00 A6 = −3.493302E+00 −1.438603E+02 5.114119E+01 −1.383566E+02 −5.949332E+01 1.389542E+02 A8 = 8.527035E+01 7.439546E+03 −1.753944E+03 3.509504E+03 3.383935E+03 −1.971735E+03 A10 = −1.705693E+03 −2.145369E+05 3.387635E+04 −6.043741E+04 −7.392323E+04 2.545067E+04 A12 = 1.353453E+04 3.644107E+06 −3.947436E+05 6.521775E+05 9.187637E+05 −2.453477E+05 A14 = −4.907557E+04 −3.623565E+07 2.656989E+06 −4.439233E+06 −6.588080E+06 1.639636E+06 A16 = 4.929382E+04 1.951413E+08 −9.396008E+06 1.885620E+07 2.724978E+07 −6.812768E+06 A18 = 0.000000E+00 −4.394361E+08 1.333982E+07 −4.505254E+07 −6.078502E+07 1.547528E+07 A20 = 0.000000E+00 0.000000E+00 0.000000E+00 4.460779E+07 5.675468E+07 −1.465264E+07 Surface # 8 9 k = −5.311763E+00 −1.493089E+00 A4 = −6.561907E+00 −5.011269E+00 A6 = 7.882206E+01 7.583999E+00 A8 = −1.393133E+03 7.209405E+01 A10 = 1.716961E+04 −5.373251E+02 A12 = −1.318552E+05 1.451806E+03 A14 = 6.270865E+05 −9.362089E+02 A16 = −1.800257E+06 −3.674457E+03 A18 = 2.861914E+06 8.300123E+03 A20 = −1.938389E+06 −5.263455E+03

The presentation of the aspheric surface formula in the third embodiment is similar to that in the first embodiment. Besides, the definitions of parameters in following tables are equal to those in the first embodiment so the repetitious details will not be given here.

The following contents may be deduced from Table 5 and Table 6.

Third embodiment (Primary reference wavelength: 555 nm) InRS41 InRS42 HVT41 HVT42 ODT % TDT % −0.01932  −0.02445  0.31867 0.45428 1.77013 0.56470 | f/f1 | | f/f2 | | f/f3 | | f/f4 | | f1/f2 | | f2/f3 | 0.10288 1.34045 0.86785 0.66150 13.02904  0.64743 Σ PPR Σ NPR Σ PPR/ | Σ NPR | Σ PP Σ NP f1/Σ PP 2.00195 0.97073 2.06231 2.90312 −13.97995  −4.30513  f4/Σ NP IN12/f IN23/f IN34/f TP3/f TP4/f −0.06862  0.08007 0.11406 0.03340 0.14094 0.16611 InTL HOS HOS/HOI InS/HOS InTL/HOS Σ TP/InTL 1.23495 1.86203 1.81131 0.85611 0.66323 0.76308 (TP1 + IN12)/TP2 (TP4 + IN34)/TP3 TP1/TP2 TP3/TP4 IN23/(TP2 + IN23 + TP3) 0.95599 1.41553 0.64641 0.84851 0.22207 | InRS41 |/TP4 | InRS42 |/TP4 HVT42/HOI HVT42/HOS PhiA4/InTL PhiA4/HOI 0.0905  0.1145  0.4419  0.2440  1.25997  1.513619 PhiA4 PhiB PhiC PhiD RI9 PhiA4/HEP 1.556 mm 1.956 mm 2.656 mm  3.106 mm 45% 2.42019 PSTA PLTA NSTA NLTA SSTA SLTA 0.019 mm 0.031 mm 0.003 mm −0.004 mm −0.002 mm 0.001 mm

The following contents may be deduced from Table 5 and Table 6.

Related inflection point values of third embodiment (Primary reference wavelength: 555 nm) HIF111 0.3425 HIF111/HOI 0.3332 SGI111 0.0566 |SGI111|/(|SGI111| + 0.2085 TP1) HIF121 0.2460 HIF121/HOI 0.2393 SGI121 0.0351 |SGI121|/(|SGI121| + 0.1402 TP1) HIF211 0.2882 HIF211/HOI 0.2803 SGI211 0.0643 |SGI211|/(|SGI211| + 0.1620 TP2) HIF221 0.3453 HIF221/HOI 0.3359 SGI221 −0.0381 |SGI221|/(|SGI221| + 0.1028 TP2) HIF311 0.2914 HIF311/HOI 0.2835 SGI311 −0.0844 |SGI311|/(|SGI311| + 0.3177 TP3) HIF321 0.2914 HIF321/HOI 0.2835 SGI321 −0.0615 |SGI321|/(|SGI321| + 0.2535 TP3) HIF411 0.1520 HIF411/HOI 0.1479 SGI411 0.0249 |SGI411|/(|SGI411| + 0.1043 TP4) HIF421 0.2081 HIF421/HOI 0.2025 SGI421 0.0410 |SGI421|/(|SGI421| + 0.1611 TP4)

The numerical related to the length of outline curve is shown according to table 5 and table 6.

Third embodiment (Reference wavelength = 555 nm) ARE/TP ARE ½(HEP) ARE value ARE − ½(HEP) 2(ARE/HEP) % TP (%) 11 0.323 0.327 0.00406 101.26% 0.215 152.13% 12 0.304 0.307 0.00375 101.24% 0.215 143.00% 21 0.323 0.333 0.01011 103.13% 0.333 100.16% 22 0.323 0.325 0.00195 100.60% 0.333  97.71% 31 0.323 0.342 0.01927 105.97% 0.181 188.85% 32 0.323 0.334 0.01080 103.34% 0.181 184.18% 41 0.323 0.327 0.00407 101.26% 0.214 153.12% 42 0.323 0.331 0.00825 102.56% 0.214 155.09% ARS ARS/TP ARS EHD value ARS − EHD (ARS/EHD) % TP (%) 11 0.383 0.390 0.00691 101.80% 0.215 181.48% 12 0.304 0.307 0.00375 101.24% 0.215 143.00% 21 0.368 0.382 0.01347 103.66% 0.333 114.79% 22 0.400 0.406 0.00635 101.59% 0.333 122.18% 31 0.425 0.450 0.02439 105.73% 0.181 248.10% 32 0.449 0.465 0.01650 103.68% 0.181 256.77% 41 0.528 0.548 0.02042 103.87% 0.214 256.56% 42 0.706 0.757 0.05157 107.31% 0.214 354.64%

The Fourth Embodiment (Embodiment 4)

Please refer to FIG. 4A, FIG. 4B, FIG. 4C, and FIG. 4D. FIG. 4A is a schematic view of the optical image capturing system according to the fourth embodiment of the present application. FIG. 4B is longitudinal spherical aberration curves, astigmatic field curves, and an optical distortion curve of the optical image capturing system in the order from left to right according to the fourth embodiment of the present application, FIG. 4C is a lateral aberration diagram of tangential fan, sagittal fan, the longest operation wavelength and the shortest operation wavelength passing through an edge of the entrance pupil and incident on the image plane by 0.7 HOI according to the fourth embodiment of the present application, and FIG. 4D is a numerical figure of relative illumination of each view field on the image plane according to the fourth embodiment of the present application. As shown in FIG. 4A, in order from an object side to an image side, the optical image capturing system includes a first lens element 410, an aperture stop 400, a second lens element 420, a third lens element 430, a fourth lens element 440, an IR-bandstop filter 470, an image plane 480, and an image sensing device 490.

The first lens element 410 has positive refractive power and it is made of plastic material. The first lens element 410 has a convex object-side surface 412 and a concave image-side surface 414, and both of the object-side surface 412 and the image-side surface 414 are aspheric. The image-side surface 414 has an inflection point.

The second lens element 420 has negative refractive power and it is made of plastic material. The second lens element 420 has a convex object-side surface 422 and a concave image-side surface 424, and both of the object-side surface 422 and the image-side surface 424 are aspheric and have an inflection point.

The third lens element 430 has positive refractive power and it is made of plastic material. The third lens element 430 has a concave object-side surface 432 and a convex image-side surface 434, and both of the object-side surface 432 and the image-side surface 434 are aspheric and have an inflection point.

The fourth lens element 440 has negative refractive power and it is made of plastic material. The fourth lens element 440 has a convex object-side surface 442 and a concave image-side surface 444, and both of the object-side surface 442 and the image-side surface 444 are aspheric and have an inflection point.

The IR-bandstop filter 470 is made of glass material without affecting the focal length of the optical image capturing system and it is disposed between the fourth lens element 440 and the image plane 480.

In the optical image capturing system of the fourth embodiment, the first and the third lens elements are positive lens elements, and focal lengths are respectively f1 and f3. A sum of focal lengths of all lens elements with positive refractive power is ΣPP. The following relation is satisfied: ΣPP=f1+f3. Hereby, it is favorable for allocating the positive refractive power of a single lens element to other positive lens elements and the significant aberrations generated in the process of moving the incident light can be suppressed.

In the optical image capturing system of the fourth embodiment, the focal lengths of the second and the fourth lens elements are respectively f2 and f4. A sum of focal lengths of all lens elements with negative refractive power is ΣNP. The following relation is satisfied: ΣNP=f2+f4. Hereby, it is favorable for allocating the negative refractive power of a single lens element to other negative lens elements.

Please refer to the following Table 7 and Table 8.

The detailed data of the optical image capturing system of the fourth embodiment is as shown in Table 7.

TABLE 7 Data of the optical image capturing system f = 1.3238 mm; f/HEP = 2.370; HAF = 37.3825 deg; tan(HAF) = 0.7641 Focal Surface # Curvature Radius Thickness Material Index Abbe # length 0 Object Plano 600 1 Lens 1 0.826378369 0.242 Plastic 1.545 55.96 2.363 2 2.059435851 0.047 3 Ape. Plano 0.054 stop 4 Lens 2 1.54316432 0.202 Plastic 1.642 22.46 −51.596 5 1.399177166 0.106 6 Lens 3 −1.190735147 0.318 Plastic 1.545 55.96 0.810 7 −0.35305323 0.029 8 Lens 4 0.839506984 0.178 Plastic 1.642 22.46 −0.990 9 0.333323218 0.137 10 IR-band Plano 0.210 BK7_SCHOTT 1.517 64.13 stop filter 11 Plano 0.370 12 Image Plano plane Reference wavelength (d-line) = 555 nm; shield position: The clear aperture of the third surface is 0.280 mm. As for the parameters of the aspheric surfaces of the fourth embodiment, reference is made to Table 8.

TABLE 8 Aspheric Coefficients Surface # 1 2 4 5 6 7 k = −1.567331E+00 1.970850E+01 −3.621785E+00 2.839174E+00 −2.497830E+01 −1.149578E+00 A4 = 1.655126E−01 −1.704701E+00 −2.312997E+00 −6.249596E−01 2.870682E−01 3.210857E+00 A6 = −5.824348E−01 −1.972977E+00 −6.927249E−01 −8.604247E+00 −1.986057E+00 −6.019237E+01 A8 = −1.182978E+01 −4.312127E+01 −1.072428E+02 6.598151E+01 −2.113580E+01 1.049823E+03 A10 = 2.172763E+02 8.464405E+02 −8.996457E+01 −7.998883E+02 1.115432E+03 −1.157197E+04 A12 = −1.738758E+03 −5.534995E+03 1.529361E+04 5.797895E+03 −7.270311E+03 7.807890E+04 A14 = −6.889623E+01 −1.786065E+03 −1.154865E+05 −2.122366E+04 −3.285153E+03 −3.109808E+05 A16 = 3.431766E+04 1.251304E+05 3.273054E+05 3.343841E+04 1.858558E+05 7.126193E+05 A18 = 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 −6.862888E+05 −8.533113E+05 A20 = 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 9.040614E+05 3.811336E+05 Surface # 8 9 k = −1.033119E+01 −5.062763E+00 A4 = −7.386775E+00 −4.681364E+00 A6 = 6.697799E+01 3.876766E+01 A8 = −4.248551E+02 −2.405526E+02 A10 = 1.485653E+03 9.983928E+02 A12 = −1.508217E+03 −2.753831E+03 A14 = −8.709124E+03 4.961749E+03 A16 = 3.811917E+04 −5.593459E+03 A18 = −6.206508E+04 3.571264E+03 A20 = 3.804853E+04 −9.839921E+02

The presentation of the aspheric surface formula in the fourth embodiment is similar to that in the first embodiment. Besides the definitions of parameters in following tables are equal to those in the first embodiment so the repetitious details will not be given here.

The following contents may be deduced from Table 7 and Table 8.

Fourth embodiment (Primary reference wavelength: 555 nm) InRS41 InRS42 HVT41 HVT42 ODT % TDT % −0.06850  0.03361 0.24561 0.46236 1.71806 0.89667 | f/f1 | | f/f2 | | f/f3 | | f/f4 | | f1/f2 | | f2/f3 | 0.56027 0.02566 1.63453 1.33656 0.04579 63.70735  Σ PPR Σ NPR Σ PPR/| Σ NPR | Σ PP Σ NP f1/Σ PP 2.19480 1.36222 1.61120 3.17268 −52.58665  0.74473 f4/Σ NP IN12/f IN23/f IN34/f TP3/f TP4/f 0.98117 0.07676 0.08034 0.02172 0.24059 0.13441 InTL HOS HOS/HOI InS/HOS InTL/HOS Σ TP/InTL 1.17701 1.89391 1.84232 0.97506 0.62147 0.79888 (TP1 + IN12)/TP2 (TP4 + IN34)/TP3 TP1/TP2 TP3/TP4 IN23/(TP2 + IN23 + TP3) 1.70136 6.64896 1.19812 1.78997 0.16968 | InRS41 |/TP4 | InRS42 |/TP4 HVT42/HOI HVT42/HOS PhiA4/InTL PhiA4/HOI 0.3850  0.1889  0.4498  0.2441  1.19965  1.373541 PhiA4 PhiB PhiC PhiD RI9 PhiA4/HEP 1.412 mm 1.812 mm 2.512 mm 2.962 mm 45% 2.52794 PSTA PLTA NSTA NLTA SSTA SLTA 0.001 mm 0.001 mm 0.009 mm 0.001 mm 0.001 mm 0.001 mm

The following contents may be deduced from Table 7 and Table 8.

Related inflection point values of fourth embodiment (Primary reference wavelength: 555 nm) HIF121 0.1624 HIF121/ 0.1580 SGI121 0.0054 |SGI121|/(|SGI121| + 0.0218 HOI TP1) HIF211 0.1433 HIF211/ 0.1394 SGI211 0.0056 |SGI211|/(|SGI211| + 0.0271 HOI TP2) HIF221 0.2248 HIF221/ 0.2187 SGI221 0.0161 |SGI221|/(|SGI221| + 0.0737 HOI TP2) HIF311 0.2380 HIF311/ 0.2316 SGI311 −0.0191 |SGI311|/(|SGI311| + 0.0565 HOI TP3) HIF321 0.3422 HIF321/ 0.3328 SGI321 −0.1411 |SGI321|/(|SGI321| + 0.3070 HOI TP3) HIF411 0.1194 HIF411/ 0.1162 SGI411 0.0068 |SGI411|/(|SGI411| + 0.0368 HOI TP4) HIF421 0.1769 HIF421/ 0.1721 SGI421 0.0345 |SGI421|/(|SGI421| + 0.1624 HOI TP4)

The numerical related to the length of outline curve is shown according to table 7 and table 8.

Fourth embodiment (Reference wavelength = 555 nm) ARE/TP ARE ½(HEP) ARE value ARE − ½(HEP) 2(ARE/HEP) % TP (%) 11 0.280 0.284 0.00430 101.53% 0.242 117.46% 12 0.279 0.278 −0.00061  99.78% 0.242 114.99% 21 0.280 0.279 −0.00058  99.79% 0.202 138.31% 22 0.280 0.280 0.00021 100.07% 0.202 138.70% 31 0.280 0.280 0.00039 100.14% 0.318  88.00% 32 0.280 0.300 0.02012 107.19% 0.318  94.19% 41 0.280 0.279 −0.00037  99.87% 0.178 157.08% 42 0.280 0.287 0.00684 102.44% 0.178 161.13% ARS ARS/TP ARS EHD value ARS − EHD (ARS/EHD) % TP (%) 11 0.280 0.284 0.00427 101.53% 0.242 117.46% 12 0.279 0.278 −0.00061  99.78% 0.242 114.99% 21 0.313 0.314 0.00048 100.15% 0.202 155.29% 22 0.402 0.402 0.00060 100.15% 0.202 199.23% 31 0.436 0.438 0.00128 100.29% 0.318 137.45% 32 0.477 0.527 0.05041 110.57% 0.318 165.55% 41 0.545 0.563 0.01799 103.30% 0.178 316.38% 42 0.713 0.737 0.02356 103.30% 0.178 414.06%

The Fifth Embodiment (Embodiment 5)

Please refer to FIG. 5A, FIG. 5B, FIG. 5C, and FIG. 5D. FIG. 5A is a schematic view of the optical image capturing system according to the fifth embodiment of the present application, FIG. 5B is longitudinal spherical aberration curves, astigmatic field curves, and an optical distortion curve of the optical image capturing system in the order from left to right according to the fifth embodiment of the present application, FIG. 5C is a lateral aberration diagram of tangential fan, sagittal fan, the longest operation wavelength and the shortest operation wavelength passing through an edge of the entrance pupil and incident on the image plane by 0.7 HOI according to the fifth embodiment of the present application, and FIG. 5D is a numerical figure of relative illumination of each view field on the image plane according to the fifth embodiment of the present application. As shown in FIG. 5A, in order from an object side to an image side, the optical image capturing system includes an aperture stop 500, a first lens element 510, a second lens element 520, a third lens element 530, a fourth lens element 540, an IR-bandstop filter 570, an image plane 580, and an image sensing device 590.

The first lens element 510 has positive refractive power and it is made of plastic material. The first lens element 510 has a convex object-side surface 512 and a concave image-side surface 514, and both of the object-side surface 512 and the image-side surface 514 are aspheric. The image-side surface 514 has an inflection point.

The second lens element 520 has positive refractive power and it is made of plastic material. The second lens element 520 has a concave object-side surface 522 and a convex image-side surface 524, and both of the object-side surface 522 and the image-side surface 524 are aspheric.

The third lens element 530 has positive refractive power and it is made of plastic material. The third lens element 530 has a concave object-side surface 532 and a convex image-side surface 534, and both of the object-side surface 532 and the image-side surface 534 are aspheric. The image-side surface 534 has an inflection point.

The fourth lens element 540 has negative refractive power and it is made of plastic material. The fourth lens element 540 has a convex object-side surface 542 and a concave image-side surface 544, and both of the object-side surface 542 and the image-side surface 544 are aspheric. The object-side surface 542 has two inflection points and the image-side surface 544 has an inflection point.

The IR-bandstop filter 570 is made of glass material without affecting the focal length of the optical image capturing system and it is disposed between the fourth lens element 540 and the image plane 580.

In the optical image capturing system of the fifth embodiment, the first, second and third lens elements are positive lens elements, and focal lengths are respectively, f1, f2 and f3. A sum of focal lengths of all lens elements with positive refractive power is ΣPP. The following relation is satisfied: ΣPP=f1+f2+f3. Hereby, it is favorable for allocating the positive refractive power of a single lens element to other positive lens elements and the significant aberrations generated in the process of moving the incident light can be suppressed.

In the optical image capturing system of the fifth embodiment, a sum of focal lengths of all lens elements with negative refractive power is ΣNP=f4.

Please refer to the following Table 9 and Table 10.

The detailed data of the optical image capturing system of the fifth embodiment is as shown in Table 9.

TABLE 9 Data of the optical image capturing system f = 1.3290 mm; f/HEP = 2.05; HAF = 37.5120 deg; tan(HAF) = 0.7677 Focal Surface # Curvature Radius Thickness Material Index Abbe # length 0 Object Plano 600 1 Ape. stop Plano −0.067 2 Lens 1 0.65717761 0.325 Plastic 1.545 55.96 1.280 3 8.979197625 0.097 4 Lens 2 −1.422865307 0.210 Plastic 1.545 55.96 1.826 5 −0.616904778 0.056 6 Lens 3 −0.353893307 0.210 Plastic 1.642 22.46 10.464 7 −0.41493791 0.030 8 Lens 4 0.849089121 0.229 Plastic 1.642 22.46 −1.524 9 0.408052782 0.099 10 IR-bandstop Plano 0.210 BK_7 1.517 64.13 filter 11 Plano 0.310 12 Image plane Plano 0.000 Reference wavelength (d-line) = 555 nm; shield position: The clear aperture of the sixth surface is 0.386 mm. The clear aperture of the seventh surface is 0.453 mm. The clear aperture of the eighth surface is 0.508 mm. The clear aperture of the ninth surface is 0.725 mm. As for the parameters of the aspheric surfaces of the fifth embodiment, reference is made to Table 10.

TABLE 10 Aspheric Coefficients Surface # 2 3 4 5 6 7 k = −3.925526E−02 1.106896E+02 8.374418E+00 −1.044020E+00 −5.014467E+00 −9.846061E−01 A4 = −1.620391E−01 −1.547662E+00 −3.589866E+00 −1.015161E+00 −3.238962E+00 3.016104E+00 A6 = −6.426520E+00 −1.998224E+00 1.100620E+01 −3.531239E+01 2.379891E+01 −1.653534E+01 A8 = 2.130092E+02 −2.696018E+02 −7.717802E+02 6.424481E+02 −2.795082E+02 1.393050E+02 A10 = −4.220815E+03 3.227346E+03 1.170138E+04 −5.587356E+03 7.013066E+03 −5.364754E+02 A12 = 4.457354E+04 −2.206555E+04 −8.273742E+04 3.109404E+04 −8.485975E+04 −2.513836E+02 A14 = −2.631628E+05 6.782040E+04 3.174330E+05 −1.029411E+05 4.432129E+05 5.043128E+03 A16 = 6.368479E+05 −2.842720E+04 −4.659187E+05 1.522332E+05 −8.642727E+05 −5.097076E+02 A18 = 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 A20 = 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 Surface # 8 9 k = −9.875459E+00 −7.073006E+00 A4 = −6.640131E+00 −2.650595E+00 A6 = 3.918441E+01 1.129569E+01 A8 = −1.688453E+02 −3.999801E+01 A10 = −4.449741E+01 9.206871E+01 A12 = 4.547368E+03 −1.330059E+02 A14 = −2.166284E+04 1.037496E+02 A16 = 3.399714E+04 −3.268016E+01 A18 = 0.000000E+00 0.000000E+00 A20 = 0.000000E+00 0.000000E+00

The presentation of the aspheric surface formula in the fifth embodiment is similar to that in the first embodiment. Besides the definitions of parameters in following tables are equal to those in the first embodiment so the repetitious details will not be given here.

The following contents may be deduced from Table 9 and Table 10.

Fifth embodiment (Primary reference wavelength: 555 nm) InRS41 InRS42 HVT41 HVT42 ODT % TDT % −0.10769  −0.04922  0.22750 0.42999 1.21497 1.18158 | f/f1 | | f/f2 | | f/f3 | | f/f4 | | f1/f2 | | f2/f3 | 1.03800 0.72797 0.12701 0.87225 0.70133 0.17447 Σ PPR Σ NPR Σ PPR/| Σ NPR | Σ PP Σ NP f1/Σ PP 1.89298 0.87225 2.17023 13.56969  −1.52366  0.09435 f4/Σ NP IN12/f IN23/f IN34/f TP3/f TP4/f 1.00000 0.07301 0.04204 0.02257 0.15834 0.17213 InTL HOS HOS/HOI InS/HOS InTL/HOS Σ TP/InTL 1.15689 1.77595 1.72758 0.96228 0.65142 0.84190 (TP1 + IN12)/TP2 (TP4 + IN34)/TP3 TP1/TP2 TP3/TP4 IN23/(TP2 + IN23 + TP3) 2.00867 1.22967 1.54664 0.91988 0.11731 | InRS41 |/TP4 | InRS42 |/TP4 HVT42/HOI HVT42/HOS PhiA4/InTL PhiA4/HOI 0.4707  0.2151  0.4183  0.2421   1.232939  1.387524 PhiA4 PhiB PhiC PhiD RI9 PhiA4/HEP 1.42637 mm 1.82637 mm 2.52637 mm  2.97637 mm 45% 2.20018 PSTA PLTA NSTA NLTA SSTA SLTA  −0.051 mm  0.050 mm  0.008 mm −0.00018 mm −0.007 mm −0.003 mm

The following contents may be deduced from Table 9and Table 10.

Related inflection point values of fifth embodiment (Primary reference wavelength: 555 nm) HIF121 0.0763 HIF121/HOI 0.0742 SGI121 0.0003 |SGI121|/(|SGI121| + 0.0008 TP1) HIF321 0.3394 HIF321/HOI 0.3301 SGI321 −0.1100 |SGI321|/(|SGI321| + 0.3433 TP3) HIF411 0.1194 HIF411/HOI 0.1161 SGI411 0.0068 |SGI411|/(|SGI411| + 0.0289 TP4) HIF412 0.4837 HIF412/HOI 0.4705 SGI412 −0.0862 |SGI412|/(|SGI412| + 0.2736 TP4) HIF421 0.1814 HIF421/HOI 0.1765 SGI421 −0.0300 |SGI421|/(|SGI421| + 0.1158 TP4)

The numerical related to the length of outline curve is shown according to table 9 and table 10.

Fifth embodiment (Reference wavelength = 555 nm) ARE/TP ARE ½(HEP) ARE value ARE − ½(HEP) 2(ARE/HEP) % TP (%) 11 0.325 0.338 0.01236 103.80% 0.325 104.00% 12 0.325 0.328 0.00289 100.89% 0.325 101.08% 21 0.325 0.345 0.01926 105.92% 0.210 164.13% 22 0.325 0.346 0.02052 106.30% 0.210 164.73% 31 0.325 0.348 0.02267 106.97% 0.210 165.42% 32 0.325 0.344 0.01880 105.78% 0.210 163.58% 41 0.325 0.326 0.00071 100.22% 0.229 142.57% 42 0.325 0.331 0.00582 101.79% 0.229 144.80% ARS ARS/TP ARS EHD value ARS − EHD (ARS/EHD) % TP (%) 11 0.337 0.350 0.01289 103.83% 0.325 107.72% 12 0.363 0.372 0.00909 102.50% 0.325 114.68% 21 0.358 0.387 0.02902 108.10% 0.210 184.30% 22 0.390 0.425 0.03493 108.95% 0.210 202.49% 31 0.386 0.421 0.03544 109.19% 0.210 200.08% 32 0.453 0.484 0.03037 106.70% 0.210 229.82% 41 0.508 0.543 0.03507 106.91% 0.229 237.25% 42 0.725 0.772 0.04656 106.42% 0.229 337.28%

The Sixth Embodiment (Embodiment 6)

Please refer to FIG. 6A, FIG. 6B, FIG. 6C, and FIG. 6D. 6A is a schematic view of the optical image capturing system according to the sixth Embodiment of the present application, FIG. 6B is longitudinal spherical aberration curves, astigmatic field curves, and an optical distortion curve of the optical image capturing system in the order from left to right according to the sixth Embodiment of the present application. FIG. 6C is a lateral aberration diagram of tangential fan, sagittal fan, the longest operation wavelength and the shortest operation wavelength passing through an edge of the entrance pupil and incident on the image plane by 0.7 HOI according to the sixth embodiment of the present application, and FIG. 6D is a numerical figure of relative illumination of each view field on the image plane according to the sixth embodiment of the present application. As shown in FIG. 6A, in order from an object side to an image side, the optical image capturing system includes an aperture stop 600, a first lens element 610, a second lens element 620, a third lens element 630, a fourth lens element 640, an IR-bandstop filter 670, an image plane 680, and an image sensing device 690.

The first lens element 610 has positive refractive power and it is made of plastic material. The first lens element 610 has a convex object-side surface 612 and a convex image-side surface 614, and both of the object-side surface 612 and the image-side surface 614 are aspheric. The object-side surface 612 has an inflection point.

The second lens element 620 has positive refractive power and it is made of plastic material. The second lens element 620 has a concave object-side surface 622 and a convex image-side surface 624, and both of the object-side surface 622 and the image-side surface 624 are aspheric and have an inflection point.

The third lens element 630 has negative refractive power and it is made of plastic material. The third lens element 630 has a concave object-side surface 632 and a convex image-side surface 634, and both of the object-side surface 632 and the image-side surface 634 are aspheric. The object-side surface 632 has an inflection point.

The fourth lens element 640 has negative refractive power and it is made of plastic material. The fourth lens element 640 has a convex object-side surface 642 and a concave image-side surface 644, and both of the object-side surface 642 and the image-side surface 644 are aspheric and have an inflection point.

The IR-bandstop filter 670 is made of glass material without affecting the focal length of the optical image capturing system and it is disposed between the fourth lens element 640 and the image plane 690.

In the optical image capturing system of the sixth embodiment, the first and the second lens elements are positive lens elements, and focal lengths are respectively f1 and f2. A sum of focal lengths of all lens elements with positive refractive power is ΣPP. The following relations are satisfied: ΣPP=f1+f2. Hereby, it is favorable for allocating the positive refractive power of a single lens element to other positive lens elements and the significant aberrations generated in the process of moving the incident light can be suppressed.

In the optical image capturing system of the sixth embodiment, a sum of focal lengths of all lens elements with negative refractive power is ΣNP. The following relations are satisfied: ΣNP=f3+f4. Hereby, it is favorable for allocating the negative refractive power of a single lens element to other negative lens elements.

Please refer to the following Table 11 and Table 12.

The detailed data of the optical image capturing system of the sixth Embodiment is as shown in Table 11.

TABLE 11 Data of the optical image capturing system f = 1.3219 mm; f/HEP = 2.05; HAF = 37.5115 deg; tan(HAF) = 0.7676 Focal Surface # Curvature Radius Thickness Material Index Abbe # length 0 Object Plano 600 1 Ape. Stop/ 0.910134564 0.297 Plastic 1.535 56.05 1.25 Lens 1 2 −2.234704553 0.146 3 Lens 2 −0.911923961 0.264 Plastic 1.535 56.05 1.65 4 −0.494882008 0.068 5 Lens 3 −0.316713012 0.181 Plastic 1.636 23.89 −3.57 6 −0.449582937 0.030 7 Lens 4 0.470694691 0.211 Plastic 1.544 56.09 −3.30 8 0.314038592 0.123 9 IR-bandstop Plano 0.210 BK_7 1.517 64.13 filter 10 Plano 0.310 11 Image plane Plano 0.000 Reference wavelength (d-line) = 555 nm; shield position: The clear aperture of the fourth surface is 0.440 mm. The clear aperture of the sixth surface is 0.530 mm. As for the parameters of the aspheric surfaces of the sixth Embodiment, reference is made to Table 12.

TABLE 12 Aspheric Coefficients Surface # 1 2 3 4 5 6 k = −1.266469E+00 2.495254E+01 2.717976E+00 −4.008969E+00 −6.300607E+00 −1.057859E+00 A4 = −5.130804E−01 −8.945288E−01 −1.398240E+00 −1.221317E+00 −4.227344E+00 2.969829E+00 A6 = −4.017185E+00 −1.875099E+00 2.428942E+01 −3.420122E+01 3.547631E+01 −1.556892E+01 A8 = 1.601752E+02 −1.180297E+02 −6.215338E+02 6.420384E+02 −1.183421E+02 1.260285E+02 A10 = −3.980061E+03 2.709061E+03 1.05158E+04 −5.621817E+03 −1.606236E+01 −5.044403E+02 A12 = 4.457354E+04 −2.206555E+04 −8.289563E+04 3.089865E+04 6.402369E+02 2.609659E+02 A14 = −2.631628E+05 6.782040E+04 3.174330E+05 −1.025962E+05 −1.041974E+03 3.703562E+03 A16 = 6.368479E+05 −2.842720E+04 −4.659187E+05 1.522332E+05 1.119349E+03 −6.938851E+03 A18 = 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 A20 = 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 Surface # 7 8 k = −9.875460E+00 −4.690981E+00 A4 = −4.061699E+00 −2.447153E+00 A6 = 1.986941E+01 1.109978E+01 A8 = −6.432516E+01 −3.827027E+01 A10 = 4.734763E+01 8.621683E+01 A12 = 4.385064E+02 −1.240440E+02 A14 = −1.672881E+03 1.008030E+02 A16 = 1.869852E+03 −3.577061E+01 A18 = 0.000000E+00 0.000000E+00 A20 = 0.000000E+00 0.000000E+00

In the sixth Embodiment, the presentation of the aspheric surface formula is similar to that in the first embodiment. Besides, the definitions of parameters in following tables are equal to those in the first embodiment, so the repetitious details will not be given here.

The following contents may be deduced from Table 11 and Table 12.

Sixth Embodiment (Primary reference wavelength: 555 nm) InRS41 InRS42 HVT41 HVT42 ODT % TDT % −0.04585  0.02741 0.33217 0.54007 1.37494 0.81780 | f/f1 | | f/f2 | | f/f3 | | f/f4 | | f1/f2 | | f2/f3 | 1.06010 0.79977 0.36983 0.40091 0.75443 0.46242 Σ PPR Σ NPR Σ PPR/| Σ NPR | Σ PP Σ NP f1/Σ PP 1.85987 0.77074 2.41309 2.89981 −6.87159  0.43001 f4/Σ NP IN12/f IN23/f IN34/f TP3/f TP4/f 0.47984 0.11048 0.05144 0.02269 0.13692 0.15967 InTL HOS HOS/HOI InS/HOS InTL/HOS Σ TP/InTL 1.19686 1.84000 1.78988 0.97417 0.65047 0.79609 (TP1 + IN12)/TP2 (TP4 + IN34)/TP3 TP1/TP2 TP3/TP4 IN23/(TP2 + IN23 + TP3) 1.68090 1.33185 1.12693 0.85756 0.13265 | InRS41 |/TP4 | InRS42 |/TP4 HVT42/HOI HVT42/HOS PhiA4/InTL PhiA4/HOI 0.2173  0.1299  0.5254  0.2935   1.211504  1.410506 PhiA4 PhiB PhiC PhiD RI9 PhiA4/HEP  1.45 mm  1.85 mm  2.55 mm   3.00 mm 50% 2.24866 PSTA PLTA NSTA NLTA SSTA SLTA −0.006 mm −0.001 mm 0.006 mm −0.00013 mm 0.001 mm 0.005 mm

The following contents may be deduced from Table 11 and Table 12.

Related inflection point values of sixth embodiment (Primary reference wavelength: 555 nm) HIF111 0.2662 HIF111/HOI 0.2590 SGI111 0.0353 |SGI111|/(|SGI111| + 0.1063 TP1) HIF211 0.3181 HIF211/HOI 0.3094 SGI211 −0.0661 |SGI211|/(|SGI211| + 0.2006 TP2) HIF221 0.4138 HIF221/HOI 0.4025 SGI221 −0.1599 |SGI221|/(|SGI221| + 0.3775 TP2) HIF321 0.3056 HIF321/HOI 0.2973 SGI321 −0.0836 |SGI321|/(|SGI321| + 0.3159 TP3) HIF411 0.1485 HIF411/HOI 0.1444 SGI411 0.0180 |SGI411|/(|SGI411| + 0.0784 TP4) HIF421 0.2040 HIF421/HOI 0.1984 SGI421 0.0474 |SGI421|/(|SGI421| + 0.1835 TP4)

The numerical related to the length of outline curve is shown according to table 11 and table 12.

Sixth embodiment (Reference wavelength = 555 nm) ARE/TP ARE ½(HEP) ARE value ARE − ½(HEP) 2(ARE/HEP) % TP (%) 11 0.323 0.327 0.00414 101.28% 0.297 110.15% 12 0.323 0.327 0.00390 101.21% 0.297 110.07% 21 0.323 0.333 0.00955 102.96% 0.264 126.18% 22 0.323 0.343 0.01980 106.13% 0.264 130.07% 31 0.323 0.345 0.02216 106.86% 0.181 190.76% 32 0.323 0.338 0.01508 104.67% 0.181 186.85% 41 0.323 0.326 0.00272 100.84% 0.211 154.38% 42 0.323 0.335 0.01235 103.82% 0.211 158.95% ARS ARS/TP ARS EHD value ARS − EHD (ARS/EHD) % TP (%) 11 0.323 0.327 0.00411 101.27% 0.297 110.15% 12 0.379 0.388 0.00905 102.39% 0.297 130.70% 21 0.403 0.417 0.01413 103.51% 0.264 158.23% 22 0.440 0.481 0.04126 109.38% 0.264 182.54% 31 0.445 0.490 0.04494 110.11% 0.181 270.45% 32 0.523 0.548 0.02481 104.74% 0.181 302.77% 41 0.611 0.648 0.03689 106.04% 0.211 307.08% 42 0.823 0.911 0.08787 110.68% 0.211 431.60%

The above-mentioned descriptions represent merely the exemplary embodiment of the present disclosure, without any intention to limit the scope of the present disclosure thereto. Various equivalent changes, alternations or modifications based on the claims of present disclosure are all consequently viewed as being embraced by the scope of the present disclosure. 

What is claimed is:
 1. An optical image capturing system, from an object side to an image side, comprising: a first lens element with refractive power; a second lens element with refractive power; a third lens element with refractive power; a fourth lens element with refractive power; and an image plane; wherein the optical image capturing system consists of four lens elements with refractive power, at least one of the four lens elements has positive refractive power, focal lengths of the four lens elements are f1, f2, f3 and f4, a focal length of the optical image capturing system is f, an entrance pupil diameter of the optical image capturing system is HEP, a distance on an optical axis from an object-side surface of the first lens element to the image plane is HOS, a distance from the object-side surface of the first lens element to the image-side surface of the fourth lens element on an optical axis is InTL, an effective maximum diameter of the image-side surface of the fourth lens element is PhiA4, a length of outline curve from an axial point on any surface of any one of the four lens elements to a coordinate point of vertical height with a distance of a half of the entrance pupil diameter from the optical axis on the surface along an outline of the surface is denoted as ARE. The following relations are satisfied: 1.2≦f/HEP≦10, 0.5≦HOS/f≦20, 0<PhiA4/InTL≦1.5 and 0.1≦2(ARE/HEP)≦2.0.
 2. The optical image capturing system of claim 1, wherein TV distortion for image formation in the optical image capturing system is TDT, a half of a diagonal of an effective detection field of the image sensing device is denoted by HOI, a lateral aberration of the longest operation wavelength of a positive direction tangential fan of the optical image capturing system passing through an edge of the entrance pupil and incident on the image plane by 0.7 HOI is denoted as PLTA, and a lateral aberration of the shortest operation wavelength of the positive direction tangential fan of the optical image capturing system passing through the edge of the entrance pupil and incident on the image plane by 0.7 HOI is denoted as PSTA, a lateral aberration of the longest operation wavelength of a negative direction tangential fan of the optical image capturing system passing through the edge of the entrance pupil and incident on the image plane by 0.7 HOI is denoted as NLTA a lateral aberration of the shortest operation wavelength of a negative direction tangential fan of the optical image capturing system passing through the edge of the entrance pupil and incident on the image plane by 0.7 HOI is denoted as NSTA, a lateral aberration of the longest operation wavelength of a sagittal fan of the optical image capturing system passing through the edge of the entrance pupil and incident on the image plane by 0.7 HOI is denoted as SLTA, a lateral aberration of the shortest operation wavelength of the sagittal fan of the optical image capturing system passing through the edge of the entrance pupil and incident on the image plane by 0.7 HOI is denoted as SSTA. The following relations are satisfied: PLTA≦100 μm; PSTA≦100 μm; NLTA≦100 μm; NSTA≦100 μm; SLTA≦100 μm; and SSTA≦100 μm; |TDT|<100%.
 3. The optical image capturing system of claim 1, wherein a maximum effective half diameter position of any surface of any one of the four lens elements is denoted as EHD, and a length of outline curve from an axial point on any surface of any one of the four lens elements to the maximum effective half diameter position of the surface along the outline of the surface is denoted as ARS. The following relation is satisfied: 0.1≦ARS/EHD≦2.0.
 4. The optical image capturing system of claim 1, wherein a half of a maximum view angle of the optical image capturing system is HAF, and the following relation is satisfied: 0 deg<HAF≦100 deg.
 5. The optical image capturing system of claim 1, wherein the optical image capturing system is satisfied: 0 mm<HOS≦15 mm.
 6. The optical image capturing system of claim 1, wherein a length of outline curve from an axial point on the object-side surface of the fourth lens element to a coordinate point of vertical height with a distance of a half of the entrance pupil diameter from the optical axis on the surface along an outline of the surface is denoted as ARE41; a length of outline curve from an axial point on the image-side surface of the fourth lens element to the coordinate point of vertical height with the distance of a half of the entrance pupil diameter from the optical axis on the surface along the outline of the surface is denoted as ARE42, and a thickness of the second lens element on the optical axis is TP2. The following relations are satisfied: 0.5≦ARE41/TP4≦20 and 0.5≦ARE42/TP/4≦20.
 7. The optical image capturing system of claim 1, wherein the optical image capturing system is satisfied: 0<PhiA4/HEP≦4.0.
 8. The optical image capturing system of claim 1, wherein a maximum height for image formation on the image plane perpendicular to the optical axis in the optical image capturing system is denoted by HOI, and the following relation is satisfied: 0<PhiA4/2HOI≦2.0.
 9. The optical image capturing system of claim 1, further comprising an aperture stop, a distance from the aperture stop to the image plane on the optical axis is InS, a maximum height for image formation on the image plane perpendicular to the optical axis in the optical image capturing system is denoted by HOI, and the following relation is satisfied: 0.2≦InS/HOS≦1.1 and 0.5<HOS/HOI≦1.6.
 10. An optical image capturing system, from an object side to an image side, comprising: a first lens element with refractive power; a second lens element with refractive power; a third lens element with refractive power; a fourth lens element with refractive power and an image plane; a first lens element positioning element including a mirror base which is hollow and opaque, and the mirror base having a cylinder and a basement which are connected with each other; the cylinder accommodating the four lens elements, the basement between the fourth lens element and the image plane, and an outer periphery of the basement greater than an outer periphery of the cylinder, and a maximum value of the minimum side length of the basement perpendicular to the surface of the optical axis denoted by PhiD; wherein the optical image capturing system consists of four lens elements with refractive power, at least one of the four lens elements with positive refractive power, an object-side surface and an image-side surface of the fourth lens element are aspheric surfaces, focal lengths of the four lens elements are f1, f2, f3 and f4, a focal length of the optical image capturing system is f, an entrance pupil diameter of the optical image capturing system is HEP, a distance on an optical axis from an object-side surface of the first lens element to the image plane is HOS, a distance from the object-side surface of the first lens element to the image-side surface of the fourth lens element on an optical axis is InTL, a length of outline curve from an axial point on any surface of any one of the four lens elements to a coordinate point of vertical height with a distance of a half of the entrance pupil diameter from the optical axis on the surface along an outline of the surface is denoted as ARE. The following relations are satisfied: 1.2≦f/HEP≦10, 0.5≦HOS/f≦20, 0 mm<PhiD≦3.3 mm and 0.1≦2(ARE/HEP)≦2.0.
 11. The optical image capturing system of claim 10, wherein a maximum effective diameter of the image-side surface of the fourth lens element is PhiA4, and the following relation is satisfied: 0<PhiA4/InTL≦1.5
 12. The optical image capturing system of claim 10, wherein a maximum effective half diameter position of any surface of any one of the four lens elements is denoted as EHD, and a length of outline curve from an axial point on any surface of any one of the four lens elements to the maximum effective half diameter position of the surface along the outline of the surface is denoted as ARS. The following relation is satisfied: 0.1≦ARS/EHD≦2.0.
 13. The optical image capturing system of claim 10, wherein a height for image formation on the image plane perpendicular to the optical axis in the optical image capturing system is denoted by HOI, a relative illumination of the HOI is denoted by R1, a lateral aberration of the longest operation wavelength of a positive direction tangential fan of the optical image capturing system passing through an edge of the entrance pupil and incident on the image plane by 0.7 HOI is denoted as PLTA, and a lateral aberration of the shortest operation wavelength of the positive direction tangential fan of the optical image capturing system passing through the edge of the entrance pupil and incident on the image plane by 0.7 HOI is denoted as PSTA, a lateral aberration of the longest operation wavelength of a negative direction tangential fan of the optical image capturing system passing through the edge of the entrance pupil and incident on the image plane by 0.7 HOI is denoted as NLTA, a lateral aberration of the shortest operation wavelength of a negative direction tangential fan of the optical image capturing system passing through the edge of the entrance pupil and incident on the image plane by 0.7 HOI is denoted as NSTA, a lateral aberration of the longest operation wavelength of a sagittal fan of the optical image capturing system passing through the edge of the entrance pupil and incident on the image plane by 0.7 HOI is denoted as SLTA, a lateral aberration of the shortest operation wavelength of the sagittal fan of the optical image capturing system passing through the edge of the entrance pupil and incident on the image plane by 0.7 HOI is denoted as SSTA. The following relations are satisfied: PLTA≦100 μm; PSTA≦100 μm; NLTA≦100 μm; NSTA≦100 μm; SLTA≦100 μm, SSTA≦100 μm, and 10%≦R1<100%.
 14. The optical image capturing system of claim 10, wherein at least one of an object-side surface and image-side surface of at least two lens elements of the four lens elements respectively has at least one inflection point.
 15. The optical image capturing system of claim 10, wherein a distance between the first lens element and the second lens element on the optical axis is IN12, and the following relation is satisfied: 0<IN12/f≦5.0.
 16. The optical image capturing system of claim 10, wherein the optical image capturing system is satisfied: 0<PhiA4/HEP≦4.0.
 17. The optical image capturing system of claim 10, wherein a maximum height for image formation on the image plane perpendicular to the optical axis in the optical image capturing system is denoted by HOI, and the following relation is satisfied: 0≦PhiA4/2HOI≦2.0.
 18. The optical image capturing system of claim 10, wherein the optical image capturing system is satisfied: 0 mm<PhiA4≦1.8 min.
 19. The optical image capturing system of claim 18, wherein at least one of the four lens elements is a light filter element with a wavelength of less than 500 nm.
 20. An optical image capturing system, from an object side to an image side, comprising: a first lens element with positive refractive power; a second lens element with positive refractive power; a third lens element with refractive power; a fourth lens element with refractive power; and an image plane; a first lens element positioning element including a mirror base which is hollow and opaque, and the mirror base having a cylinder and a basement which are connected with each other; the cylinder accommodating the four lens elements, the basement between the fourth lens element and the image plane, and an outer periphery of the basement greater than an outer periphery of the cylinder, and a maximum value of the minimum side length of the basement perpendicular to the surface of the optical axis denoted by PhiD; and a second lens element positioning element accommodated in the mirror base and including a positioning part and a connecting part; the positioning part being hollow and directing contacting and accommodating any of the four lens elements, facilitating the lens elements being aligned on the optical axis, the connecting part disposed outside the positioning part and directly contacting an inner periphery of the cylinder, and a maximum diameter of the connection part perpendicular to the surface of the optical axis denoted by PhiC; wherein the optical image capturing system consists of four lens elements with refractive power, at least one lens element of the four lens elements with positive refractive power, and an object-side surface and an image-side surface of the fourth lens element both are aspheric, a maximum effective diameter of the image-side surface of the fourth lens element denoted by PhiA4, focal lengths of the four lens elements are f1, f2, f3 and f4, a focal length of the optical image capturing system is f, an entrance pupil diameter of the optical image capturing system is HEP, a distance on an optical axis from an object-side surface of the first lens element to the image plane is HOS, a distance from the object-side surface of the first lens element to the image-side surface of the four lens element on an optical axis is InTL, a length of outline curve from an axial point on any surface of any one of the four lens elements to a coordinate point of vertical height with a distance of a half of the entrance pupil diameter from the optical axis on the surface along an outline of the surface is denoted as ARE. The following relations are satisfied: 1.2≦f/HEP≦10, 0.5≦HOS/f≦20, PhiC<PhiD, 0 mm<PhiD≦3.3 mm and 0.1≦2(ARE/HEP)≦2.0.
 21. The optical image capturing system of claim 20, wherein the optical image capturing system is satisfied: 0<PhiA4/InTL≦1.5.
 22. The optical image capturing system of claim 20, wherein the optical image capturing system is satisfied: 0<PhiA4/HEP≦4.0.
 23. The optical image capturing system of claim 20, wherein a maximum height for image formation on the image plane perpendicular to the optical axis in the optical image capturing system is denoted by HOI, and the following relations are satisfied: 0<PhiA4/2HOI≦2.0.
 24. The optical image capturing system of claim 20, wherein the optical image capturing system is satisfied: 0 mm<PhiA4≦1.8 mm.
 25. The optical image capturing system of claim 20, wherein the optical image capturing system further comprise an aperture stop, an image sensing device and a driving module, the image sensing device is disposed on the image plane, a distance from the aperture stop to the image plane is InS, and the driving module couples with the two lens elements to displace the lens elements. The following relation is satisfied: 0.2≦InS/HOS≦1.1. 